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PERFORMANCE AND RECOUERY UNDER<br />

PROLONGED<br />

VIBRATION<br />

TAREK ííl. KHALIL, B.IYl.E., (Yl.S. in I.E<br />

by<br />

A DISSERTATION<br />

IN<br />

INDUSTRIAL<br />

ENGINEERING<br />

Submitted to the Graduate Faculty<br />

of Texas Technological College<br />

in Partial Fulfillment of<br />

the Requirements for<br />

the Degree of<br />

DOCTOR OF PHILGSOPHY<br />

Approved


t (S- /<br />

No.-"^ ^•-<br />

(2. uii.''. t2..y<br />

ACK^jüÜli •.nr:ílE')T5<br />

í am cje.jnly i-irieíitra to ür . (T!. '^ Ayoub fjr hii"^<br />

direntior o^ thio disc^ertatlon and t.ú tt^ Í otrer members<br />

oí^ my ?.dv.isoiy conmittee, Drs, Richarc^ A. Dudek, Jeny<br />

D. Rarrsey, Brisn K. Lamberl, and Charles G. Halccib, r or<br />

their helpful advice. Ifianks alço gü te Hflr. James L.<br />

Cibbs for hir, assistance in ::onstruction of the equipi.ent.<br />

This research luas supported by THEIYIIS Contract No.<br />

DAAD05-59-C-01Ü2, betujeen the U.S. Department oF Defense<br />

and Texas Technological College, R. A. Dudek, Project<br />

lYlanager. The contents do not necessarily reflect the official<br />

opinion or policy of the Department of Defense or the<br />

Department of the Army. Reproduction is authorlzed for any<br />

purpose of the U.S. Government.<br />

11


ACKNOliJLEDGIYlENTS<br />

LIST OF TABLES<br />

TABLE OF CONTENTS<br />

Page<br />

ii<br />

v/i<br />

LIST OF ILLUSTRATIÜNS v/iii<br />

Chapter<br />

I. INTRÜDUCTIGN 1<br />

Statement of the Problem 1<br />

Purpose and Scope 4<br />

Revieu; of Literature and Previous Research, , 5<br />

Sources of Vibration and Typical<br />

Frequencies , 7<br />

Subjective Reactions to Uibration<br />

and Tolerance Limits . . , . , 10<br />

Simulation of Human Subjects 17<br />

lYIechanical Simulation of Human<br />

Response to Uibration 19<br />

Effects of Vibration upon Performance , . 27<br />

Tracking Tasks 28<br />

l/ibration Effects upon Vision, Visual<br />

Acuity and Reaction Time 32<br />

Vibration Effect upon (Ylotor Performance<br />

and Body Configuration , , , 36<br />

Summary 38<br />

II. EXPERIfriENíAL EQUIPIYIENT AND flílE ASUREíílEN T 39<br />

Equipment for íílaintaining the Independent<br />

Variables 39<br />

iii


: \j<br />

Page<br />

Vibration Platform 39<br />

Accelerometers 40<br />

Equipment for lYleasuring the Dependent<br />

Variables 45<br />

Performance Console 45<br />

Hand Rest and Control Assembly Device . . . . 46<br />

Seat 48<br />

Signal Playing Apparatus 48<br />

Change of Polarity Circuit 50<br />

Analog Computer 50<br />

Dynagraph Recorder 53<br />

Supporting Equipment for Controlling<br />

the Variables • 56<br />

Signal Recording Apparatus 56<br />

UJide Range Oscillator 56<br />

ITlagnetic Tape Recorder 59<br />

Earphones 59<br />

lYieasuremen t 59<br />

III.<br />

EXPERIfílENTAL DESIGN 61<br />

The Task 61<br />

The Variables ..... 66<br />

Independent Variables 66<br />

The Dependent Variables ..... 75<br />

The Controlled Variables 77<br />

Statistical Design of the Experiment ...... 79


V<br />

Pjge<br />

First Analysis of Variance "9<br />

Second Analysis of Variance ^ 1<br />

Third Analysis of Variance 63<br />

Subjects , 83<br />

Experimental Routine 84<br />

Safety Precautions . 88<br />

IV. FINDINGS AND INTER PRETAT lON S 91<br />

First Analysis of Variance Results 92<br />

Second Analysis of Variance Results 113<br />

Third Analysis of Variance Results 117<br />

V. CONCLUSIONS AND RECOmnflENDAT lONS 127<br />

Conclusions 127<br />

Environmental Effects ..... 127<br />

Period Effect 126<br />

Effect of Ujork/Rest Schedule<br />

by Period Interaction 129<br />

Effect of UJork/Rest Schedule upon<br />

Increase of Error Score due to Vibration<br />

• 132<br />

Transmissibility of Vibration ...... 134<br />

Subjective Reaction to Vibration 135<br />

Recommendations for Further Research .... 135<br />

Summary • 139<br />

BIBLIOGRAPHY 141<br />

APPENDIX 155


LIST OF TABLES<br />

Table<br />

Page<br />

1. Summary of Factors 80<br />

2. Expected Hílean Square for Experimental Design . , 82<br />

3. Subject Information . , 84<br />

4. ANOVA for Absolute Error Score (Normal and<br />

Vibrational Environment) 93<br />

5. lYleans and Standard Deviation of Environment<br />

Effect on Absolute Error Score (Normal<br />

and Vibrational Environments) 94<br />

6. (Yleans and Standard Deviations of Period<br />

Effect on Absolute Error Score (Normal<br />

and Vibrational Environment) . . . . . . . . 94<br />

7. ííleans and Standard Deviation of UJork/Rest<br />

by Period Interaction Effect on Error<br />

Score (Normal and Vibrational Environment). , 99<br />

8. ANOVA for Difference in Average Error Score<br />

(Vibration and Recovery) . , , 113<br />

9. (Yleans and Standard Deviations of UJork/Rest<br />

Schedule Effect on Difference in Average<br />

Error Score (Vibration and Recovery) 114<br />

10. ííleans and Standard Deviations of Period<br />

Effect on Difference in Average Error<br />

Score (vibration and Recovery) 116<br />

11. ANOVA for Difference in Average Error<br />

Score (Vibration) 119<br />

12. lYleans and Standard Deviations of UJork/Rest<br />

Schedule Effect on Difference in Average<br />

Error Score (Vibration) 119<br />

13. ANOVA for Percentage Increase in Error Score<br />

(Vibration) 120<br />

vi


VI 1<br />

Pige<br />

14. (yleans and Standard Deviations of UJork/Rest<br />

Schedule Effect on Percentage Increase<br />

in Error Score (Vibration) 122<br />

15. Natural Frequencies for Various Parts of the<br />

Body 156<br />

16. Specifications of the Accelerometers Used<br />

in this Study 157<br />

17. Calculation of the G Levei Transmitted 158


LIST GF ILLUSTRATIÜNS<br />

Figure<br />

Page<br />

1. Average acceleration measured under operational<br />

conditions for commercial and<br />

military vehicles 9<br />

2. "Short-time" tolerance curves and "long-time"<br />

recommended limits 16<br />

3. The simplest model of the human body is a<br />

one-mass-spring system luith damping 21<br />

4. Parallel and series models for duplicating<br />

the humar> body impedance 21<br />

5. The modulus of the impedance of one subject<br />

at varied body postures compared luith the<br />

impedance of a purê mass (muj) and of a<br />

one-mass-spring system ujith damping 24<br />

6. Phase angle of the impedance for one subject<br />

at varied body postures compared luith<br />

phase angle of a one-mass-spring system<br />

luith damping 24<br />

7. The vibration platform drive mechanism ..... 41<br />

8. Accelerometer mounted on vibration platform ... 43<br />

9. Accelerometer mounted on subject's hip and<br />

vibration stop button 43<br />

10. Accelerometer mounted on subject's head and<br />

earphones 44<br />

11. Accelerometers, amplifiers, pouer supply and<br />

suiitch 44<br />

12. Cathode ray tube and signal lights 47<br />

13. Signal playing apparatus, change of polarity<br />

Circuit, vibration platform activator<br />

and signal siuitch 47<br />

Vlll


IX<br />

Paqe<br />

14. Hand rest and control assembly device 49<br />

15. Subject's controlling position 4?<br />

16. Schematic of the CRT sujeep circuit 51<br />

17. Schematic of the change of polarity circuit ... 52<br />

18. Schematic of the analog computar integrating<br />

circuit 53<br />

19. Vieuj of the analog computer shouiing integrating<br />

circuit connections . 54<br />

20. Dynagraph recorder 55<br />

21. Signal recording apparatus, oscillator<br />

and voltmeter 57<br />

22. Tape recorder, oscillator and voltmeter 57<br />

23. Voltage regulator 58<br />

24. Vieuj of signal and vibration monitoring<br />

equipment 58<br />

25. Generalized illustration of a continuous<br />

closed-loop man-machine system; such<br />

Systems usually are referred to as<br />

tracking systems 63<br />

26. Vieuj of signal recording apparatus shouiing<br />

cem profile 64<br />

27. Recordings on a dynagraph recorder chart .... 65<br />

28. Selected u/ork/rest schedules 69<br />

29. Performance on tracking tasks in relation<br />

to "long time" recommended limits ...... 72<br />

30. Vibration facility 85<br />

31. Subject^s station 89<br />

32. Experimenter station 89


X<br />

Pago<br />

33. Plot of means of absolute error score versus<br />

environment<br />

34. Plot of means of absolute error score versus<br />

period<br />

35. Plot of means of absolute error score versus<br />

uiork/rest period interaction<br />

36. Plot of means of absolute error score versus<br />

period—UJ/R schedule I<br />

37. Plot of means of absolute error score versus<br />

period—UJ/R schedule II<br />

38. Plot of means of absolute error score versus<br />

period—UJ/R schedule III<br />

39. Plot of means of absolute error score versus<br />

period—UJ/R schedule IV<br />

40. Plot of average error score versus time—<br />

Ul/R schedule I<br />

41. Plot of average error score versus time—<br />

UJ/R schedule II<br />

42. Plot of average error score versus time—<br />

UJ/R schedule III<br />

43. Plot of average error score versus time—<br />

UJ/R schedule IV<br />

44. Plot of means of difference in average error<br />

score versus uiork/rest schedule (vibration<br />

and recovery)<br />

45. Plot of means of difference in average error<br />

score versus period (vibration and<br />

recovery) .<br />

46. Plot of means for difference in average error<br />

score versus uiork/rest schedule (vibration) .<br />

47. Plot of means for percentage increase in error<br />

score versus ujork/rest schedule (vibration) .<br />

48. Recording of a subject's hip acceleration<br />

before and during task performance<br />

95<br />

96<br />

98<br />

100<br />

101<br />

102<br />

103<br />

106<br />

107<br />

108<br />

109<br />

115<br />

118<br />

121<br />

123<br />

125


XI<br />

49. Typical response of monitoring accelerometers . .<br />

50. Example learning curve obtained for subject<br />

number 5 during six experimental trials. . . .<br />

51. Plot of absolute error score versus minute<br />

readings—UJ/R schedule I<br />

52. Plot of absolute error score versus minute<br />

readings—UJ/R schedule II<br />

53. Plot of absolute error score versus minute<br />

readings—Uj/R schedule III .<br />

54. Plot of absolute error score versus minute<br />

readings—UJ/R schedule IV<br />

age<br />

158<br />

159<br />

160<br />

161<br />

162<br />

163


CHAPTER I<br />

INTRODUCTION<br />

Statement of the Problem<br />

UJith the increasing sophistication of our society's<br />

technology, ever greater concern is being accorded the<br />

concept of system design.<br />

The criterion of success in<br />

design is usually the overall performance of the system,<br />

or system output.<br />

Recently conslderable interest has been manifested<br />

in the application of the concept to man-machine systems.<br />

An understanding of both man*s capacity and limitations,<br />

and the factors affecting them, is essential in designing any<br />

successful man-machine system.<br />

This is especially true since<br />

the occurrence of recent developments in Space, industrial<br />

and military situations, in u/hich man, the monitor link in<br />

any man-machine system, must perform efficiently for long<br />

periods of time.<br />

Such a situation has been encountered in<br />

many modern systems and u/ill be met Uíith in future ones;<br />

situations in luhich personnel cannot be added or exchanged<br />

during extended spans of time, and in luhich, during these<br />

interims, highly efficient performance by creuj members is<br />

of the utmost importance.


Adopting a definite ujork/rest schedule throughojt<br />

UJhich operators' phases of ujork and rest ensure a high<br />

probability of efficient work performance, is one solution<br />

to this problem. UJork/rest schedules have been investigated<br />

in situations in ujhich durations of missions luere thirty<br />

hours or more, and the requirement for each ujas around the<br />

clock performance of one or more tasks.<br />

Some environmental<br />

factors, such as vibration, impose limitations upon man's<br />

safe exposure period.<br />

For example, an hour of continuous<br />

vibration such as is experienced during many missions, is<br />

considered a long period of exposure at certain<br />

frequencies<br />

and leveis of acceleration (g). (Íílaintaining high levei<br />

performance by means of the most efficient u/ork/rest schedules<br />

for creui members during missions is of serious concern<br />

to system designers.<br />

Vibration is one of the basic problems confronting<br />

the design engineer.<br />

It is usually imparted from surrounding<br />

equipment to its operator or to the occupant of a vehicle<br />

or space.<br />

UJhen man is operating a vehicle, whether on the<br />

ground, the sea, or in Space, he is exposed to vibration.<br />

The vibratory conditions may last as long as the mission<br />

itself and the vibrational effect upon the operator may be<br />

a major limiting factor in obtaining<br />

the highest levei of<br />

performance from the system.<br />

The effects of vibration upon human performance are<br />

particularly<br />

relevant to military and industrial situations.


and have not yet been ujell investigated.<br />

Basic research,<br />

including a study of the effects of intersessions as wall<br />

as intrasessions of vibration, is believed to be greatly<br />

needed.<br />

either.<br />

The nature of recovery is not well investigatea,<br />

The term "recovery" here may include task as well<br />

as environmental recovery.<br />

Hopefully, an understanding of<br />

the nature of recovery will lead to better system designing.<br />

In discussing the importance of investigating<br />

the<br />

problem of performance and recovery under vibration<br />

Johnston<br />

says (1969):<br />

Performance decrements during and immediately<br />

following exposure to whole-body vibration and<br />

time for complete recovery are not cleariy defined.<br />

Although comfort leveis have been fairly well<br />

established, and recently much work has been done<br />

on performance effects, little work has been done<br />

in relating the duration of vibration exposure to<br />

human performance and in studying the recovery period<br />

following vibration exposure.<br />

Analysis of performance as a function of the duration<br />

of vibration is not well developed in the literature, while<br />

postvibration and previbration periods are seldom even<br />

discussed.<br />

Of those who did discuss some of these points, were<br />

Harris and Shoenberger<br />

(1955), who said:<br />

In addition, studies should be undertaken to<br />

determine the effects of long-term vibration. It<br />

is possible that an adaptation effect takes place<br />

by the individual learning to overcome the mechanical<br />

interfering effects of vibration; however, it is also<br />

possible that the individual becomes more sensitive<br />

to vibration due to fatigue. In fact, both adaptation<br />

and sensitization may occur at times in both experimental<br />

and operational situations.


Harris and Shoenbercer also emphasized the need<br />

for investigating intiasecsional and intersessional<br />

effects of vibration in studies of long-term situations.<br />

To provide greater insight regarding some of<br />

the problems discussed above, it is evident that some<br />

basic research is required.<br />

It is hoped that the present<br />

study will affect a contribution to the subject, and that<br />

its results may be applicable to practlcal situations.<br />

One such application is the designing of a crew work/rest<br />

schedule for the achievement of best performance during<br />

a mission.<br />

Another might be in military and commercial<br />

situations in which vibration may cease, while a pilot,<br />

for instance, must continue working or aiming for a further<br />

short period of time.<br />

Purpose and Scope<br />

/ The purpose of this research was to study the<br />

performance and recovery characteristics of man when subjected<br />

to relatively long periods of whole-body, vertical<br />

vibration.<br />

The effects of a work/rest schedule and environment<br />

on performance and recovery were investigated,<br />

Analysis<br />

of the performance in terms of the duration of vibration<br />

exposure was also undertaken.


The vibration environment under investigation is<br />

in the low-frequency range.<br />

Specific points of interest<br />

and investigation are:<br />

1. Vertical vibration<br />

2.<br />

3.<br />

Vibration frequency of 5 cps<br />

Constant amplitude of 0.08 inches<br />

displacement of 0,16 inches)<br />

(total<br />

4.<br />

5.<br />

Vibration intensity levei of about 0.20g<br />

Vibration exposure time up to 60 minutes<br />

The entire experiment was accomplished by simulating<br />

a certain mission requiring that a vertical tracking<br />

(performance<br />

measuring) task be monitored at different times<br />

during the mission, according to a specified work/rest<br />

schedule. j Further discussion will occur later in this<br />

study.<br />

The task was performed in both a normal controlled<br />

environment, and in a low-frequency vibration environment,<br />

where man-task system was subjected to the vibrational<br />

stress.<br />

Review of Literature and Previous Research<br />

A brief definition of vibration and of the terminology<br />

employed in its study is believed pertinent, and<br />

will be given; after which a review of the literature and<br />

of previous research will be pursued.<br />

The two common modes of vibration are sinusoidal<br />

vibration and random vibration.<br />

Sinusoidal vibration is


the motion of a body or system that is repeated after a<br />

given interval of time known as the period (Church, 1964).<br />

The number of cycles of motion per unit of time is called<br />

the frequency.<br />

The maximum displacement from equilibrium is<br />

the "amplitude" of vibration.<br />

The total travei is twice<br />

the amplitude and is usually referred to in the literature<br />

as double amplitude (DA).<br />

Sinusoidal vibration may be<br />

classified into two types and along various axes.<br />

The<br />

present study deals with a steady state vertical vibration.<br />

Random vibration is one in which the frequency and amplitude<br />

do not show except as a statistic, and only the probability<br />

of future occurrence can be stated.<br />

The acceleration<br />

of random vibration is usually expressed in average<br />

measures such as root-mean-square (RdflS) associated with<br />

bands of frequency componente (Holland, 1967).<br />

A vibratory<br />

system may be comprised of a mass, a spring and/or<br />

damper, or a number of these together.<br />

Every system has<br />

a natural frequency, and, in addition, a forced frequency<br />

upon application of externai force.<br />

If the frequency of<br />

the externai excitation is the same as the natural frequency,<br />

resonance takes place.<br />

Resonance in this research<br />

is taken to mean an amplification of the input acceleration<br />

by the human body.<br />

The number of natural frequencies<br />

is equal to the number of coordinates, or degrees of freedom<br />

specifying the system.<br />

A system with one degree of<br />

freedom is characterized by one resonant frequency.


The review of tine literature ojill proceed by tne<br />

steps shown below:<br />

1. Sources of vibration and typical frequencies<br />

2. Subjective effects and tolerance limits<br />

3. (Tílechanical representation of the human<br />

body transmission<br />

4. Effects of vibration upon performance<br />

Sources of Vibration<br />

and Typical Frequencies<br />

Early man was not concerned, apparently, with<br />

minor vibrational conditions existing in his environment.<br />

Uj'hen he experienced oscillatory disturbances while walking,<br />

running, riding on an animal, or even in a conveyance<br />

after he invented the wheel, he was still unaware of the<br />

effects of these oscillations upon his well-being and the<br />

efficiency of his performance.<br />

It was not until recent<br />

technological advancements and increased variety in forms<br />

of both transportation and stationery machinery that he<br />

became aware of and concerned about the problem of vibration.<br />

One aspect of this concern pertained to physiological<br />

well-being, the relationship between this and vibration<br />

becoming apparent when Clayberg<br />

(1949) indicated the effects<br />

of rough driving upon the spine and supporting structures.<br />

Fishbein and Salter (1950) lent further credence to this<br />

view.<br />

Another aspect of concern was that of impairment<br />

of man's performance upon his subjection to vibration, an


o<br />

observation with which many investigators were in accord,<br />

as will be elaborated upon later.<br />

(ílorrow (1963) indicated that there was a general<br />

agreement about the equipment situation in which shock and<br />

vibration are to be expected.<br />

He listed the most important<br />

of these situations as follows:<br />

1. Handling<br />

2. Transportation by trucks or similar vehicles<br />

3. Transportation by train<br />

4. Transportation or use in piston-engined manned<br />

aircraft<br />

5. Transportation or use in manned jet aircraft<br />

6. Use in missiles involving pulse jet, ram jet,<br />

or rocket engines<br />

7. Blasts from nuclear and other bombs, and from<br />

guns<br />

As applied to humans, such conditions and similar ones<br />

during use of Space vehicles, and equipment developed for<br />

exploration of Space, will arise.<br />

Types of shock or vibration<br />

may differ; consequently, effects upon man*s physiological<br />

well-being and performance may be varied.<br />

Investigators have tried to specify the different<br />

frequencies and other vibrational conditions to which man<br />

is subjected in the foregoing situations. Radke (1958),<br />

in discussing vehicular vibration, maintained that only<br />

vibration under 10 cps may be considered a ride problem.<br />

The higher frequencies are easily and generally attenuated.<br />

He classified commercial and military vehicle vibrations<br />

into frequency ranges between 1 and 10 cps.<br />

Figure 1 shows<br />

the average acceleration of earth moving equipnent measured<br />

under operational conditions.<br />

Holland (1967) maintained


2.0<br />

1.8<br />

FREQUENCY RAr^uE<br />

RUBBER TIRED<br />

EARTH (Y10Vn\IG<br />

EQUIPÍTIENT<br />

1.6<br />

1.4<br />

FREQUEfgCV RANGE<br />

FARnf TRACTORS &<br />

HIGHUJAY TRUCKS<br />

CJ<br />

QC<br />

LLJ<br />

>J<br />

UJ<br />

LJ<br />

et<br />

1.2<br />

1.0<br />

5 0.8<br />

HIGHUJAY<br />

TRUCK<br />

• RUBBER TIRED EARTH<br />

ílflOVI'\IG EQUIPiyiENT<br />

O TRACK TYPE TRACTORS<br />

CI> FARíll<br />

TRACTORS<br />

tr<br />

LJ<br />

0.6<br />

EQUENCY RANGE<br />

ACK TYPE TRACTORS<br />

0.4<br />

0.2<br />

O<br />

4 5 6<br />

FREQUENCY,<br />

CPS<br />

8 10<br />

Fig. 1.—Average acceleration measured under<br />

operational conditions for commercial and military<br />

vehicles. (Adapted from Harris and Crede, 1961)


10<br />

that the range of frequencies from 1 to 6 cps corresponus<br />

roughly to frequency response characteristics of aircraft..<br />

Seris and Auffret (1965) found that helicopter occupants<br />

experience vibration of frequencies varying from 1 to 35<br />

cps, with the range of frequency from 2 to 6 cps causing<br />

the maximurr^ disturbance and the greatest difficulty in<br />

devising<br />

protection.<br />

It is to be noted that in almost ali vehicles the<br />

man functions in a seated position. This position, according<br />

to Radke (1958), robs him of his own natural vibration<br />

attenuators: his legs. The seat, moreover, may amplify<br />

the vehicle motion. The degree to which this is true<br />

depende, of course, upon many other factors, such as the<br />

type of seat and its transmissibility<br />

Subjective Reactions to Vibration<br />

and Tolerance Limits<br />

A number of investigations have been made in an<br />

effort to determine subjectively either the tolerance frequency<br />

and amplitude limits of vibration, or the threshold<br />

of sensation. These investigations, although yielding<br />

different results, are in reasonable agreement insofar as<br />

general trends are concerned. A comprehensive review of this<br />

subject will be given here because of its relevance to this<br />

study and ali other studies relating to vibrational stress.<br />

ÍKIallock (1902) found that an amplitude of one onethousandth<br />

of an inch, and a frequency of 10 cps, comprises


11<br />

a source of annoyance.<br />

He maintained that an acceleratiof<br />

as low as 0.01 g is noticeable, and becomes unpleasant<br />

when it reaches 0.05 g.<br />

lYlelville (1903) suggested a formula to be used in<br />

calculating leveis of annoying vibration.<br />

According to<br />

his formula, a frequency of about 1.67 cps, and an amplitude<br />

of one inch, is considered an annoying vibration.<br />

Digby and Sankey (1911) suggested that susceptibility<br />

to vibrations depends upon velocity.<br />

Reiher and (Ifleister (1931) investigated several<br />

amplitudes and frequencies and their relationship to degree<br />

of human susceptibility, classifying their results into<br />

the following zones:<br />

1. Imperceptible<br />

2. Just perceptible<br />

3. Easily Noticeable<br />

4. Annoying<br />

5. Unpleasant<br />

6. Painful<br />

Subjects were tested while standing or lying down on the<br />

vibrating platform.<br />

Reiher and (Tleister maintained that vertical vibration<br />

is more noticeable than horizontal vibration of the same<br />

intensity, when the body was in the supine position.<br />

Jacklin<br />

(1933), in a pioneer study, used subjective<br />

judgments as relating to seated people.<br />

He confined his


12<br />

observations to three easily distinguishable reactions:<br />

1. Perceptible: one feels that he is moving, or<br />

that distant objects are moving<br />

slightly.<br />

2. Disturbing: one notes that certain organs<br />

or parts of his body vibrate more than his<br />

total body, and tries to prevent<br />

this condition<br />

by tightening certain muscles.<br />

3. Uncomfortable: one wishes very little of<br />

this treatment.<br />

Jacklin analyzed several thousand observations upon<br />

the reaction of humans to vibrations, working with a platform<br />

and soft automobile seats.<br />

From the results, he<br />

computed a combined index of "riding<br />

comfort."<br />

Helberg and Sperling<br />

(1941) experimented with<br />

leveis of frequency ranging from 1 to 2 cps and amplitudes<br />

of up to one inch.<br />

They constructed a chart of comfort<br />

zones.<br />

Janeway (1948) recommended these definite limits<br />

of vertical vibration as comfortable for humans:<br />

1. Low Frequency Range, f=l to 6 cps constant<br />

maximum<br />

"jerk" limits.<br />

ar^- 2<br />

i.e., the sensation of vibration depends upon the<br />

rate of change of acceleration.<br />

At the tolerable limit the<br />

relationship between magnitude and acceleration<br />

can be<br />

expressed as the above formula.


13<br />

2. (Yliddle Frequency Range, f « 6 to 20 cps, the<br />

limit is dependent upon accalaration, and the relationship<br />

between magnitude and frequency is<br />

af^ = 1/3<br />

3. High Frequency Range f « 20 to 60 cps, the<br />

limit appearlng to be directly proportional to the velocity<br />

of the movement. Constant maximum velocity limit<br />

af » 1/60<br />

UJhere f •« frequency in cycles per second, and a = displacement<br />

(amplitude) in inches.<br />

These limits were based upon subjective judgment of<br />

vibration.<br />

Goldman (1948) reportrd average peak accelerations<br />

at various frequencies at which<br />

1. Subjects perceive vibration<br />

2. Find it unpleasant<br />

3. Refuse to tolerate it further.<br />

Exposure time was 5 to 20 minutes. The Goldman<br />

studies were oriented toward the automotiva passenger.<br />

Brock (1956) constructed a chart, similar to the<br />

one given by Reiher and ITIeister, basing it upon vertical<br />

sinusoidal vibrational excitation.<br />

Gorrill and Snyder (1957) instructed five subjects<br />

to judge the levei of vibration while performing a tracking<br />

task. These subjects were air crewmen. They wore full flight<br />

gear and were restrained by leg belts and shoulder harnesses.


14<br />

They were asked to<br />

define:<br />

1. Probable detection of vibration<br />

2. Probable maximum operating time.<br />

They were exposed to vibrational severities varying<br />

between<br />

frequencies of from 3 to 30 cps,<br />

Ziegenruecker and (Iflagid (1959) used<br />

reinforced<br />

seats, lap belts and shoulder harnesses to strap their<br />

subjects. The latter were asked to define the limit of<br />

sinusoidal acceleration at different frequencies to which<br />

a rider would be willing to go before it seemed that actual<br />

bodily harm might occur. Short time tolerance curves were<br />

reported in this<br />

study.<br />

llflagid and Coermann<br />

(1960) subjected 15 individuais<br />

to vibrations to test for the acceleration<br />

(in g units)<br />

which they could tolerate in a seated position. Three<br />

durations of tolerance were determined, namely, "short time,"<br />

one minute, and three minutes.<br />

The subject was restrained<br />

Uiith seat belt and shoulder strap. Sinusoidal excitation<br />

was applied at various frequencies with increasing amplitude<br />

at 0.75 millimeters per second<br />

(DA) until he reported his<br />

belief that bodily harm would result from further increase.<br />

The results indicated a minimal short time tolerance of<br />

between four and eight cycles per second, at accelerations<br />

of between 1.5 and 2.0 g.<br />

Parks (1961) used 16 physically fit maie subjects to<br />

derive subjective, standardized leveis of reaction to vibration


15<br />

Four leveis were determined:<br />

1. Definitely perceptible<br />

2. lYlildly annoying<br />

3. Extremely annoying<br />

4. Alarming<br />

The leveis were significantly different, and each<br />

varied in acceleration as a function. of frequency.<br />

Linder<br />

(1962) studied personal threshold curves<br />

for vertical vibration proposed by Lippert, Janeway, Gorrill,<br />

Ziegenruecker and lYlagid and others.<br />

He then composited a<br />

curve which he recommended as an upper design limit for<br />

not more than one hour's continuous exposure of an individual<br />

under the most extreme predicted conditions.<br />

This curve<br />

is shown in Figure 2, which also summarizes the tolerance<br />

curves extracted from some of the prevlously mentioned<br />

studies.<br />

Harris, et ai. (1965), taking a more conservative<br />

attitude, suggested that LindBr's curve is too high for<br />

one hour of continuous exposure, throughout the frequency<br />

range.<br />

They suggested a lower tolerance curve, which is<br />

shown in Figure 2.<br />

Chaney<br />

(1964), utilized the descriptive leveis of<br />

Parks to establish a series of subjective curves demonstrating<br />

the response of seated subjects to sinusoidal vibration.<br />

He<br />

compared<br />

the curves obtained in his studies with those


/<br />

16<br />

\<br />

2.0<br />

1.0<br />

\<br />

^<br />

i<br />

^ V \\<br />

V ^ ^ ' ^^ Short Time<br />

One r/lin. (íYlagid,et ai.)<br />

\ \<br />

/ •<br />

Three ÍTlin.<br />

\ \<br />

/<br />

\ ^ / /<br />

\ ^^^^ I<br />

\ f \\ I y^<br />

Alarming<br />

(Parks)<br />

LD<br />

.5<br />

^./<br />

o:<br />

cr<br />

Ul<br />

CJ<br />

(_)<br />

C l<br />

.2<br />

\<br />

\<br />

\<br />

\<br />

\<br />

^>^ ^—*. One Hour or Less (Linder)<br />

et<br />

UJ<br />

a<br />

^ One Hour or Less<br />

"^ (Harris & Shoenberger)<br />

.1<br />

Long Time Tolerance Curve<br />

For (Tlilitary Aircraft (UJADC)<br />

.05<br />

\<br />

Prolonged Exposure (Janeway)<br />

.02<br />

^...^-<br />

I I 1 1 1 1 1 i<br />

O 6 8 10 12 14 16 18 20<br />

FREQUENCY (CPS)<br />

Fig. 2. — "Short-time"tolerance curves and "longtime"<br />

recommended limits. (From Harris and Shoenberger,<br />

1965)


17<br />

obtained by Gold.T,ann, (yiagic, et ai. , Gorrill and Snyder, and<br />

Parks and Snyder studies.<br />

Studies on human subjective reaction to vibration<br />

produced different results depending, of course, upon the<br />

conditions and restrictions of the study.<br />

Several investigators<br />

tried to relate these studies and combined their own<br />

results with them to reach a compromise levei of subjective<br />

reactions.<br />

It appears that in spite of the individual<br />

efforts of many investigators in this field there is no<br />

clear cut definition<br />

for leveis of subjective response.<br />

No serious attempts were made, either, for issuing standard<br />

data upon the recommended leveis of vibration in different<br />

situations and the limits that should be considered in<br />

design situations.<br />

The studies provided the means, however,<br />

of selecting the vibration leveis and the safe exposure time<br />

limits used in this experiment.<br />

Simulation of Human Subjects<br />

Experimenters cannot afford to subject their human<br />

subjects to leveis of shock and vibration which might affect<br />

their well-being.<br />

In order to detect tolerance limits and<br />

injury leveis, however, it is important to run experiments<br />

possessing various degrees of potential hazard. Animais are<br />

used first for detailed physiological studies, then with a<br />

reasonable probability, safe limits for human subjects are<br />

deduced from these studies, Goldman and Von Gierke (1961)<br />

criticize this procedure for its obvious limitations:


18<br />

The different structure, size, and weight of<br />

most animais shift their response curves to mechanical<br />

forces into other frequency ranges and to other<br />

leveis than those observed on humans.<br />

Of course, this is besides the known physiological<br />

differences between species.<br />

Still, if good scaling laws<br />

are established, studies on animais can be useful.<br />

Animais<br />

as mice, pigs and dogs are commonly<br />

used.<br />

Anthropometric dummies<br />

(sometimes called anthropomorphic)<br />

are widely used in current research.<br />

They are<br />

especially useful in aviation and automotivo crash research<br />

and for evaluating protective seats and harnesses.<br />

The anthropometric dummies approximate the human<br />

body in size, form, mobility, total weight, and weight distribution<br />

in body segments (Hertzberg, 1958). Even resiliency<br />

of the skin is simulated by some kind of padding.<br />

Static and dynamic properties of the human body are simulated<br />

by these dummies, but in somewhat crude fashion.<br />

Specific parts of the body, such as the head, brain and<br />

bonés, for example, may be and have been simulated.<br />

Cadavers<br />

were frequently used to study the static and dynamic strength<br />

of ligaments and muscles, and breaking strength of bonés.<br />

Generalized results obtained by use of dummies and other<br />

artificial simulatory objects should be accepted with great<br />

caution as applied to human subjects.


19<br />

(Tlechanical Simulation of Human<br />

Response to VibratidlT<br />

The human body, by its very structure, has a<br />

built-in vibration isolation capacity.<br />

The bony skeleton,<br />

the structure of the vertebral column and the tough,<br />

flexible ligaments and pads connecting<br />

the different parts<br />

of the body possess the ability<br />

to absorb a portion of<br />

the vibrational energy.<br />

The visceral organs contained<br />

within the thoracic cage and abdominal cavity can slide<br />

freely over each other.<br />

The kidneys, the heart and the<br />

brain are held in place by ligamentr surrounded by paddings,<br />

tissues and liquids.<br />

The human body, in short, is a very<br />

complicated<br />

system of masses, elasticities and viscous<br />

dampeners, each connected to the other.<br />

Using mechanical systems, attempts were made to<br />

simulated human response,<br />

The objective was to use the<br />

resultant data to calculate quantitatively<br />

the transmission<br />

and dissipation of vibratory energy through human body<br />

tissue; to estimate vibration amplitudes and pressures at<br />

different locations in or on the body; and to predict the<br />

effectiveness of various protective measures<br />

(Goldman and<br />

Von Gierke, 1961),<br />

For cases in which detailed quantitativo<br />

investigations are lacking, this Information may serve as<br />

a guide in the explanation of observed phenomena, or the<br />

predictlon of results.<br />

In order to calculate the transmission and dissipation<br />

of vibratory energy in the human body<br />

quantitatively,


most of the experimenters assumed that the body is a linear,<br />

20<br />

passive mechanical system<br />

(passivo elements uf a system<br />

being inertia, stiffness and damping factors). Experimenters<br />

concentrated their work upon, also, the effects<br />

of low frequency externai vibrations of the order of<br />

between<br />

,5 to 20 cps, a levei at which man*s built-in<br />

vibration isolation ability is least effective (ílflagid and<br />

Coermann, 1963),<br />

They approached the problem in two ways:<br />

by analyzing<br />

the factors involved in the transmission of<br />

vibrations to various parts of the body, such as the hips,<br />

shoulders and head; and by measuring the body*s mechanical<br />

impedance,<br />

The problem in determining the mechanodynamic<br />

properties of the human body is to find how many degrees<br />

of freedom it has, or how many lumped parameters must be<br />

found in order to predict the response of the system to<br />

the excitation applied. Coermann (1963), approaching the<br />

problem from the impedance point of view, considered the<br />

human body in both the sitting and standing positions, and<br />

treated the forces acting upon the longitudinal axis of<br />

the body.<br />

He constructed a simple model of the human body<br />

consisting of a one-mass spring system, with damping<br />

(Figure 3).<br />

In order to enhance understanding of this and<br />

other models discussed, some basic definitions are set out.<br />

Impedance is defined as the ratio of the transmitted<br />

force to the velocity at the point where force is applied.


21<br />

XI<br />

...... ///A<br />

Fig. 3.—The simplest model of the human body is<br />

a one-mass-spring system with damping. (Adapted from<br />

Coermann, 1963)<br />

(Ylj^ + (YI2 = total body weight<br />

^1<br />

(YI2 =<br />

Wnj^ « 5 Hz<br />

u^ni '<br />

.08 (yij^<br />

1 •<br />

0,30<br />

5 Hz<br />

"'n2 =<br />

(«2 = frii<br />

1 • 10,5 Hz<br />

.318<br />

Uin2 - 10 Hz<br />

2 =<br />

2 = 0,15<br />

,129<br />

^y/////////////y/y/<br />

/ / / / / / / / /<br />

(Kl<br />

Fig, 4,—Parallel and series models for duplicating<br />

the human body impedance, (Adapted from Phillips, 1969)


22<br />

For the simplified model shown in Figure 3 (Coermann,<br />

1963) the modulus of the impedance is given by<br />

2 =-^<br />

The phase angle of z is given by:<br />

tan (f<br />

(z)<br />

1 - n^ (1 - 6^^)<br />

n o<br />

and the formula for the impedance is composed of the values<br />

of the impedance of a purê mass:<br />

mass = mx<br />

X<br />

_<br />

mXgO)<br />

x^w<br />

= moj<br />

where:<br />

5: = rate of change of distance<br />

P = Force transmitted<br />

m = mass<br />

k = spring elasticity<br />

(stiffness)<br />

c = damping constant<br />

z = the mechanical<br />

impedance<br />

n = f = Frequency of the forced vibration<br />

fg undamped national frequency<br />

to<br />

O)<br />

o<br />

Ô =<br />

0) =<br />

damping factor of the system =<br />

27rf<br />

ü)Qm<br />

(O O = 27Tfo =/ k<br />

m


23<br />

Dieckman<br />

(1957,1958) determined the maximum transmission<br />

factor (ratio of movement of the body to the movement<br />

of the platform) for subjects exposed to vibration in<br />

both the vertical and transversa directions.<br />

Head/table,<br />

shoulder/table and hip/table transmissibility factors were<br />

determined.<br />

Von Bekesey (1939), Dieckman (1958), and Agate<br />

(1963) studied the effects of and responses to vibration<br />

transmitted from the hand tool to the arm and body.<br />

Abrams<br />

and Suggs (1968) applied known vibrational inputs to the<br />

hands and measured the resulting vibrations at various<br />

points on the skeletal structures. Latham (1957), also,<br />

studied transmissibility to different parts of the body and<br />

at different frequencies,<br />

It was observed that below approximately 2 cps the<br />

body acts as a unit mass.<br />

Resonance for a standing man<br />

occurred at about 5 and 12 cps and for a sitting<br />

man at<br />

between 4 and 6 cps.<br />

Calculating the impedance values (modulus and phase)<br />

allows the calculation of the transmitted energy.<br />

Figures<br />

5 and 6 show one of the impedance studies.<br />

A solid mass has an impedance of mco (mass X angular<br />

acceleration).<br />

A simple mass spring system with viscous<br />

damper has one resonant frequency.<br />

The human being reacts<br />

similarly to a complex mass spring system with two resonant<br />

peaks at 5 and 11 cps (iDagid and Coermann, 1963).<br />

From


24<br />

6 .<br />

( JD<br />

1 O<br />

-H<br />

M<br />

X<br />

0}<br />

U<br />

c<br />

(D<br />

T3<br />

fD<br />

a<br />

E<br />

•—(<br />

E<br />

U<br />

"V^<br />

u<br />

Q)<br />

to<br />

X<br />

0)<br />

c<br />

>><br />

TD<br />

2 ,<br />

O<br />

5 10<br />

Frequency - cps<br />

standing erect<br />

sitting erect<br />

one-mass—spr ing<br />

system<br />

^ y<br />

sitting reiaxed<br />

Fig. 5.—The modulus of the impedance of one subject<br />

at varied body postures compared with the impedance of a purê<br />

mass (moj) and of a one-mass-spring system with damping.<br />

(Adapted from Coermann, 1953)<br />

-30'<br />

sitting erect<br />

one-mass-sprinq system<br />

yy<br />

y>standin g erect<br />

O<br />

(D<br />

—i<br />

Dl<br />

C<br />

et<br />

(D<br />

(O<br />

(O<br />

JI<br />

CL<br />

30<br />

60<br />

\ sitting<br />

V reiaxed<br />

Subject R. C,<br />

íyiass: 84,000 dyne x sec2/c m<br />

90<br />

5 10<br />

Frequency - cps<br />

15 20<br />

Fig, 6,—Phase angle of the impedance for one subject<br />

at varied body postures compared with phase angle of a oneass-spring<br />

sytem with damping. (Adapted from Coermann, m<br />

1963)


25<br />

both resonant peaks the effective masses, elasticities,<br />

and damping<br />

factors for tí ese frequencies can be calculated.<br />

Goldman and Von Gierke<br />

(1961) noticed that the<br />

impedance and the transmissibility<br />

factors are changed<br />

considerably by individual differences in the body, its<br />

posture, and the type of support lent by a seat or back<br />

rest to a sitting<br />

subject.<br />

Coermann, et ai., suggested that the human body<br />

acts as a unit mass up to 2 cps.<br />

From 2 to 100 cps it<br />

acts as a lumped parameter system of masses, elasticities<br />

and dampers,<br />

They developed a mechanical analogue for the<br />

human body that will represent the resonance frequency of<br />

the torso, the thorax, abdômen and other parts of the body,<br />

Coermann constructed, also, several curves for the mechanical<br />

impedance of humans in sitting and standing positions,<br />

and in different postures (Coermann, 1963),<br />

Other investigators analyzed the human body in<br />

different ways. Payne (1962) examined a two degrees of<br />

freedom linear mass spring system, and Toth<br />

(1966) proposed<br />

an eight-degrees of freedom non-linear mass spring model.<br />

Liu and llflurray (1956) studied a continuum model<br />

consisting of a visco-elastic rod with a mass at the upper<br />

end.<br />

Coermann, in his attempt to relate impedance resonance<br />

to body segment motion by using a two degrees of


26<br />

freedom system, concluded that two mechnnical systems in<br />

parallel could accurately duplicata the impedance modulus.<br />

Phillips (1958) suggested, instead, duoücation of man' s<br />

mechanical impedsnce by a series of mechanical systems.<br />

UJittman<br />

(1967), in another study, maintained that<br />

a series representation of elements might be more applicable<br />

in establishing an analogy between biological and<br />

externai force responses (Figure 4, page 21).<br />

Suggs and Abrams (1968) suggested a human simulator<br />

which would possess the average dynamic properties of a<br />

population of individuais, and could be exposed to vibration<br />

inputs hazardous to man.<br />

They suggested using such a device<br />

to test various types of vehicle seats and other devices<br />

with which acceleration may be hazardous.<br />

The interesting<br />

aspect of this simulator was its design, in which the heavier<br />

mass represents the head and chest,<br />

The masses are uncoupled,<br />

in that they are each attached to a rigid frame analogous<br />

to the relatively stiff spinal column, rather than to each<br />

other.<br />

As demonstrated in this review, conslderable interest<br />

has developed in the simulation of human subjects by mechanical<br />

or other analogs,<br />

Although no efficient model has yet<br />

been found, the results obtained from some research seem<br />

reasonably encouraging,<br />

If such an analog is found, it will<br />

help to explain the response of the humans to different<br />

leveis of vibration,<br />

Transmissibility studies are of


27<br />

comparable importance,<br />

It is believed that extra work is<br />

needed in order to correlate the transmissibility<br />

factor<br />

and human performance,<br />

In this study the transmission of<br />

the vibration<br />

stress from the platform to the hip and the<br />

head was recorded with platform vibration adjusted to 5 cps<br />

(the body resonant frequency as indicated in the above<br />

studies),<br />

Effects of Vibration upon<br />

Performance<br />

The harmful effects of vibration have been studied<br />

for years, researchers having investigated the effects of<br />

vibration upon the various parts of the body as well as<br />

its total physiological effect.<br />

None of these studies<br />

revealed the exact mechanical reasons for these effects.<br />

To enable the design and system engineers to improve<br />

the vibrational environment, the testing of human performance<br />

in this environment was necessary,<br />

Specific<br />

answers had to be found as to how man is affected by vibration<br />

in varying situations,<br />

It was natural as a result of<br />

advances in Space achievements and military equipment to<br />

start experimenting with tasks of vital importance in these<br />

sectors, such as tracking efficiency, reaction time and<br />

visual abilities in reading displays and dials.<br />

Extensive<br />

research was done in these fields and others, and conflicting<br />

results were obtained in some instances,<br />

These are<br />

believed to be mainly due to the different conditions of<br />

control under which each experiment was run.


28<br />

Following<br />

is a brief review of some of the experiments<br />

in these fields and the results obtained from each,<br />

Tracking<br />

Tasks<br />

In studying tracking tasks under vibration, Gorrill<br />

(1957) used frequencies of 3 to 30 cps with acceleration<br />

up to 2.5 g in a vertical tracking task.<br />

Durations of<br />

exposure constituted a function of the tolerance levei.<br />

He<br />

found a significant decrement in performance at 15 cps and<br />

1,5 g, (Tlozell and UJhite (1958), using frequencies from<br />

8 to 25 cps and double amplitudes of 0.05, 0.1 and 0,16 inches,<br />

found no significant differences for either frequency or<br />

amplitude on vertical tracking performance,<br />

Duration of<br />

trials was two minutes, with four minute rests between trials,<br />

Their results were unpredlctable, and contradict those obtained<br />

from other studies mentioned herein for the same<br />

leveis of frequency and amplitudes.<br />

Analyzing the results<br />

of their experiment, Harris<br />

(1965) concluded that the task<br />

was an easy one and not greatly affected by some loss of<br />

visual acuity,<br />

It would seem, therefore, to be quite easy<br />

to explain<br />

the difference between this study and most other<br />

studies of tracking<br />

performance,<br />

Schmitz<br />

(1959) reported decrement in performance in<br />

a horizontal tracking task,<br />

He used vertical vibration of<br />

0,18 and 0,3 g at frequencies of 2,5 cps, Duration of<br />

trials was 90 minutes.<br />

In another study of 30 minutes<br />

exposure and vertical vibration of 0.15, 0.25 and 0,35 at


29<br />

frequencies from 0,9 to 6.5 cps, he found significant decrements<br />

in tracking performance with increase in frequency<br />

and amplitude,<br />

Ashe<br />

(1960) used frequencies of 2,4, 6, 8, 11, and<br />

16 cps, and double amplitudes of 0,055 and 0,13 (0.03 to<br />

1.4 g). For a 20 minute exposure he found significant<br />

decrements at ali frequencies at 0.13 inch (DA).<br />

Besco<br />

(1961) found significant decrements in performance<br />

under simulated turbulance, with "gusts" at 2 ft/<br />

sec Rins and 4 ft/sec RdílS.<br />

Frazer, et ai,, (1961) explored the effect of amplitude,<br />

and of plane of vibration as well as the difference,<br />

if any, between<br />

tracking on a vibrating and a non-vibrating<br />

display,<br />

Two runs of 60 seconds duration were made under<br />

each of four frequencies from 4 to 12 cps and four amplitudes<br />

of 0,063, 0,125, 0.189 and 0,250 inches,<br />

Decrement in performance<br />

was observed, as related to plane and to function<br />

of amplitude modified by a fractional exponent of frequency,<br />

Greatest decrements were noted with vertical vibration and<br />

a vertical tracking<br />

component.<br />

UJorking with the Bostrom Corporation, Hornick (1961)<br />

reported some decrement in horizontal tracking<br />

performance<br />

under vibration,<br />

In another study for the same corporation, Simons<br />

and Hornick<br />

(1961) performed an experiment in which the<br />

subjects were required to perform a task for flfteen minutes


30<br />

without vibration,<br />

The shake table was then activated for<br />

thirty minutes and performance measures were again taken,<br />

A fifteen minute post-vibration period was employed to<br />

determine recovery effects.<br />

Frequencies ranged from 1,5 to<br />

5,5 cps, with intensities of 0.15, 0,25, and 0.35 g. For<br />

compensatory<br />

tracking under vertical vibration they reported<br />

that time is the only significant factor,<br />

That is, vibration<br />

generally causes a decrement in tracking ability, and<br />

"the recovery of this ability is not complete<br />

following<br />

exposure" for the duration of the recovery period considered,<br />

They reported, also, effects upon body sway, reaction time,<br />

foot pressure and peripheral vision,<br />

Parks<br />

(1961), also, found significant decrement in<br />

performance for vertical compensatory<br />

tracking, but not for<br />

horizontal,<br />

Exposures were for four minutes, with five trials<br />

per day.<br />

Catterson, et ai,, (1962) ran a study to clarify the<br />

relative importance of changes in frequency as opposed to<br />

changes in amplitude, in determining the severity of wholebody<br />

vibration in the veftical plane, The task was twodimensional<br />

compensatory tracking, Operator performance was<br />

compared, under six frequencies from 2 to 15 cps and two<br />

amplitudes of 0,13 and 0,25 inches<br />

(DA), as a measure of the<br />

effective severity of a given levei of vibration,<br />

Five<br />

subjects performed the task in two five-minute intervals<br />

of time, while experiencing vibration for twenty minutes.


31<br />

Buckhout<br />

(1964) studied tracking performance at<br />

frequencies of 5,7 and 11 cps at peak acceleration<br />

values<br />

which were equal to 25^, 3Q',o and 35^o of the one minute<br />

tolerance levei given by (Ylagid, Coermann and Ziegenrueker,<br />

Decrements in vertical tracking performance ranged from<br />

34^ to 74^ over the control trials, Harris, et ai,, (1964)<br />

extended this experiment for the 5 cps levei under different<br />

acceleration leveis (Figure 29, page 72).<br />

Statistically significant results began at 0,20 g,<br />

Another interesting<br />

result was that subjects* performance<br />

improved through each of five trial testing periods,<br />

Trials<br />

were three minutes in length and five trials were presented<br />

during 20 minutes of continuous vibration,<br />

Holland (1967) investigated the tracking performance<br />

during long-term random vibration.<br />

Performance measures<br />

were taken during the first forty-five minutes of each hour,<br />

of a six hour session, He found that tracking performance<br />

over a period of time was remarkably stable,<br />

Average tracking<br />

performance differed slightly over the entire six hours,<br />

Tracking on the horizontal axis was found to be superior to<br />

•vertical tracking<br />

performance,<br />

Several other investigators studied tracking performance<br />

under vibration. Among them are Dolkas (1965),<br />

UJoods (1967), UJeisz (1965), Forbes (1960) and others.<br />

The<br />

majority of the experiments agreed in their evidence that<br />

tracking performance is impaired by vibration.<br />

The studies


32<br />

variec in their explanations of the factors influencing the<br />

tracking decrement, as well as in leveis of frequency,<br />

amplitude, or time elapsed which miyht have caused this<br />

decremen t.<br />

As is evident in the above review numerous experiments<br />

were performed to detect the effect of vibration on<br />

tracking performance.<br />

To draw a general conclusion from<br />

these studies is very difficult.<br />

The diverse purposes behind the many studies of<br />

tracking performance gave rise to great differences in the<br />

controlled variables tested; consequently, varying results.<br />

rhe one conclusion that one might draw is that<br />

vibration in general produces a decrement in tracking performance.<br />

This decrement is more likely to occur if the<br />

body resonates.<br />

Tracking is utilized in this experiment as a performance<br />

measuring task.<br />

Vibration Effects upon Vision, Visual<br />

Acuity and Reaction Time<br />

Coermann (1939) investigated the effects of vibration<br />

during several tasks.<br />

Visual acuity was the only thing which<br />

seemed to be adversely affected.<br />

Dennis (1965) used a frequency range of 5 to 90 cps<br />

with accelerations of 0.25 and 0.50 g in a visual performance<br />

experiment which required twelve subjects to read two digit<br />

numbers.<br />

Error scores increased by an average of 55% for


33<br />

the 0,50 g and 25% for the 0.25 g, compared with a novibration<br />

control period.<br />

Response time increased by 3^ for<br />

the 0,25 g and 12^ under 0.50 g acceleration,<br />

Hornick<br />

(1961) performed a series of studies on<br />

reaction time and visual acuity, In one study he investigated<br />

the human response to red signal lights under vertical<br />

sinusoidal vibration at a frequency of 3,5 cps and acceleration<br />

of 0.30 g, Trials were twenty minutes long. He found<br />

that response time was slower after vibration,<br />

During a<br />

second study in which he required his subjects to respond to<br />

light signals and judge Landolt Rings, he found that reaction<br />

time was slower after than during vibration, but that visual<br />

acuity was not affected,<br />

Hornick obtained almost the same<br />

results in a third study, in which trials were fifteen<br />

minutes long, but found that while peripheral vision was<br />

affected, this was only by side-to-side vibration,<br />

Loeb (1954) used frequencies of 15 cps at 0.068<br />

and 0.112 inches DA 25 cps at 0.034 and 0.056 inches DA,<br />

and 35 cps at .030 and .054 inches DA. For the exposure time<br />

of two and one-half hours, while visual acuity<br />

decreased<br />

with vibration, frequencies did not effect a significant<br />

difference. Aiming tremor increased significantly with<br />

vibration.<br />

Schmitz, in his experiments<br />

(1959,1960), demonstrated<br />

that frequencies did not affect reaction time. Reaction time<br />

was longer following vibration, but visual acuity was not<br />

affected.


34<br />

íílozell (1958), in a reading digits experiment, found<br />

no effect of amplitude, but significant effect of frequency.<br />

Frequency ranges were from 8 to 50 cps, and amplitudes were<br />

of 0.05 and .1 inch DA.<br />

Trials were two minutes and seventeen<br />

seconds long.<br />

Lewis<br />

(1943) concluded that vibration at a frequency<br />

of 20 cps with 0.04 and Q.OOt amplitudes has no effect upon<br />

response time during operation of a (Iflashburn apparatus, a<br />

control stick and rudder bar device manipulated in response<br />

to changes in three banks of lights,<br />

Imposing noise upon<br />

the vibration did not affect the response time,<br />

Lange and Coermann<br />

(1962), in a study of visual<br />

acuity under vibration, concluded that maximum<br />

decrements<br />

occurred at body resonant frequencies,<br />

(líleasurement after<br />

the cessation of vibration showed residual effects of it up<br />

to 12 cps,<br />

Shoenberger<br />

(1968) investigated dial reading performance<br />

while wearing a NASA prototype Apollo helmet,<br />

The<br />

results showed significant decrement in dial reading performance<br />

during vibration which were differentially<br />

related<br />

to the direction of vibration, frequency of vibration, and<br />

to conditions of wearing the helmet with a liner or with<br />

no liner,<br />

Dudek and Clemens (1965), investigating the effect<br />

of vibration upon certain psychomotor responses, concluded<br />

that the reaction<br />

time was not affected by vibration as


35<br />

compared with the control period.<br />

They used frequencies<br />

of 4, 8 and 12 cps,<br />

Johnston<br />

(1969), in an experiment on the effects of<br />

vibration on body orientation, however, measured the reaction<br />

time for twenty maie subjects before, during and after<br />

vibration, using frequencies of O, 2, 5 and 8 cps, and<br />

concluded that the reaction time is significantly slower<br />

within a vibratory environment, as compared with before<br />

and after vibration time periods,<br />

The frequency of the<br />

vibration had no significant effect upon reaction time,<br />

Research on the effects of vibration on visual acuity<br />

showed that in general visual acuity is suffered by low<br />

frequency vibration,<br />

Greater decrements in visual acuity<br />

occurs at frequency values near the body resonance,<br />

These<br />

general statements, although pointing to certain trends in<br />

performance, have little practlcal value in specific design<br />

situations,<br />

Research concernlng human reaction time is not as<br />

conclusivo as it is hoped to be in same,<br />

This is probably<br />

true because of the different situations at which reaction<br />

time was measured and due to a lack of agreement between the<br />

studies in defining the exact time periods of pre-vibration,<br />

vibration and post vibration,<br />

The research in visual acuity is pertinent to this<br />

research because it has been argued that decrements in


36<br />

tracking performance occurs due to a loss of visual acuity<br />

under vibrational stress.<br />

Vibration Effect upon íYlotor Performance<br />

and Body Configuration<br />

Dudek and Clemens (1965) investigated the influence<br />

of vertical vibration, within the limits encountered under<br />

typical industrial conditions, upon performance of various<br />

elements of total cycle time in the cases of certain<br />

types<br />

of hand motions. Three different switches requiring three<br />

distinct types of motion were to be operated by twentyseven<br />

maie subjects,<br />

Frequencies of 4, 8 and 12 cps, and<br />

amplitudes of 0,15, 0.2 and 0,25 inches were used,<br />

The<br />

investigators concluded that the speed of flexion and extension<br />

movements is not affected by vibration,<br />

The variation<br />

in frequency, apparently, affects the supination movement<br />

to a greater degree than it affects either the extension<br />

or the flexion movements,<br />

Bush<br />

(1966) investigated the effects of low-level,<br />

vertical vibration upon the performance of a sensory<br />

inputphysical<br />

response task which requires a decision<br />

factor,<br />

He used frequencies of 3, 4, 5, 6 and 7 cps, and amplitudes<br />

of ,05 and ,10 inches,<br />

Three seating configurations were<br />

used to investigate the effect of varied seating<br />

configurations<br />

in modifying any performance decrement<br />

resulting<br />

from the vibration,<br />

Bush concluded that within the scope<br />

of his experiment, relative decrement in performance


37<br />

accuracy will result from low-level vibration with increments<br />

in amplitude,<br />

The seating configuration is a determinant<br />

of performance in a low-level dynamic environment,<br />

Chaney and Parks (1964) investigated the effect of<br />

vibration on visual-motor performance in the cases of subjects<br />

who had to operate several controls of different shapes and<br />

sizes,<br />

The type of control had no effect upon accuracy of<br />

performance under vibration,<br />

Using a motor performance task, Larue (1965) concluded<br />

that man can achieve accuracy leveis under vibration,<br />

equal to those he can achieve in a normal environment, as<br />

long as the frequency is higher than 5 cps,<br />

Johnston (1959) investigated the effects of lowfrequency<br />

vibration upon whole body orientation in both<br />

sitting and standing body configurations,<br />

He subjected<br />

twenty maie individuais to frequencies of O, 2, 5 and 8 cps,<br />

and an amplitude of 0,09 inch,<br />

Vibration exposure times<br />

were twenty minutes,<br />

and after vibration,<br />

He measured performance before, during<br />

Johnston concluded that time to orient<br />

toward a target, which he called travei time, increases significantly<br />

as frequency increases, and that accuracy is<br />

affected.<br />

Travei time is shorter in a clockwise direction,<br />

and in a standing, rather than a sitting, body configuration.<br />

The duration of vibration exposure had no significant effect<br />

in Johnston's study.


38<br />

Summary<br />

The results of the above mentioned investigations<br />

indicate that vibration caures a general feeling of discomfort<br />

when applied for a long period of time or at a high<br />

levei of acceleration (g levei). Vibration in general<br />

causes decrement in performance, especially around the<br />

frequencies of the whole-body resonance.<br />

This review of the literature reveals several<br />

points of interest which have yet to be investigated with<br />

sufficient thoroughness,<br />

The effects of prolonged vibration<br />

were not extensively discussed in the literature; neither<br />

the intersessional or intrasessional effects of vibration<br />

are well investigated; and recovery from vibration, or<br />

the post-vibration period, is an área which needs further<br />

research,<br />

Questions in these provinces constituted the<br />

impetus for this research.


CHAPTER<br />

II<br />

EXPERIITIENTAL<br />

EQUIPÍYIENT AND lYlEASUREÍYIENT<br />

The equipment used in this experiment is divided<br />

into three different categories, namely, the equipment for:<br />

1, Íílaintaining the independent variables<br />

2, lYleasuring the dependent variables<br />

3, Supporting control of variables<br />

Equipment for 'flain taining the<br />

Independent Variables<br />

Vibration<br />

Platform<br />

A vibration platform which was built by the Department<br />

of Industrial Engineering at Texas Tech served as the<br />

control over the vibrational environment, On the platform,<br />

a mechanical shake table, four feet square and fourteen<br />

inches above the floor, a performance console and a seat<br />

were mounted, The upper portion of the table was mounted<br />

on four springs, one at each corner, Restraints at each<br />

corner limited the horizontal, or transversa, movement to<br />

plus or minus 0,01 inch, thus providing for a single degree<br />

of freedom (vertical) vibration, A simple cam mechanism<br />

provided the forcing function, This mechanism is composed<br />

of an inner eccentric pressed onto the drive shaft, and an<br />

39


40<br />

outer eccentric which, when rotated on the inner eccentric,<br />

provides any amplitude from zero to approximately 0.2 inch.<br />

The cam shaft and its drive train were mounted on the base<br />

section of the platform. Force was transmitted to the<br />

upper portion of the table (the moving section) through<br />

ball-bearing pillow blocks, The cam shaft was driven by<br />

a one-half horsepower variable speed electric motor through<br />

a series of accurately turned pully and V-belts (Figure 7),<br />

The forcing function operated directly through the midpoint<br />

of the platform, with the seat mounted immediately over<br />

this área in such a way that the force was transmitted<br />

through the general location of the center of gravity of<br />

the subject's upper trunk, Before experimentation with<br />

each subject, the platform was balanced by adding lead<br />

weights, A scribed wheel built into the platform permitted<br />

speed adjustment of the motor, A generator tachometer was<br />

installed within the platform and a voltmeter attached to<br />

the outside, providing the means of adjusting motor speed,<br />

consequently<br />

frequency,<br />

Accelerometers<br />

The accelerometer is an electromechanical transducer<br />

which produces at its output terminais an e,m,f. proportional<br />

to the acceleration to which the transducer is subjected<br />

Three accelerometers, manufactured by the Bruel and<br />

Kjaer Company, in Copenhagen, Denmark, and marketed in


Fig. 7, — The vibration olatform drive mechanism<br />

41


42<br />

Clevelana, Ghio, i^-ere used, They are of the B & K 4332<br />

piezoelectric compression type. Acceleration was monitored<br />

at three different points: tne vibration platform; the<br />

subject's hip; the subject's head. Figures 8, 9 and 10<br />

give the positions in which the accelerometers were muunted,<br />

Those for the hip and head were housed in small pieces of<br />

styrofoam, to prevent any uncomfortable abrasion of the<br />

subject's body, The head accelerometer was attached by<br />

a variable length strap, Each accelerometer has its own<br />

specifications, Table 15, Appendix B, shows those for the<br />

accelerometers used in this study,<br />

The output signals of the accelerometers were routed<br />

through separate amplifiers, Those used were of the Bruel<br />

and Kjaer 2624 chargé type, and each accelerometer had its<br />

own amplifier, These were powered by a supply unit of the<br />

Bruel and Kjaer type 2805, which operates on 28 volts, The<br />

accelerometers, amplifiers and power supply unit are shown<br />

in Figure 11,<br />

The output of the amplifiers was controlled by a<br />

switching knob which was connected to a dynograph recorder,<br />

Through this arrangement, the output of any of the accelerometers<br />

was recorded upon turning the switch to its particular<br />

amplifier, The switch was used to reduce the number of<br />

channels which the accelerometers would have used, had they<br />

been connected directly to the recorder.


43<br />

Fig. 8.—Accelerometer mounted on vibration platform<br />

Fig. 9.—Accelerometer mounted on subject*s hio<br />

and vibration stop button


44<br />

Fig. 10.—Accelerometer mounted on subject's head<br />

and earphones.<br />

Fig, 11.—Accelerometers, amplifiers, power<br />

and svuitch.<br />

SUDDI/


45<br />

Equipment for (Ifloasurinq the<br />

Dependent Variables<br />

Performance Console<br />

A Performance Console was constructed according to<br />

the human engineering standards given in the handbooks.<br />

It<br />

was mounted rigidly on the vibration platform in order to<br />

provide a man-task vibration system,' In the middle of the<br />

front panei of the console a cathode ray tube<br />

(CRT) was<br />

mounted,<br />

It was snugged tightly into a soft synthetic<br />

material which acted as a cushion protecting the tube from<br />

any motion which might be caused by the vibration of the<br />

whole device,<br />

The CRT was secured, also, by belts and<br />

supported by the front and back of the console panei,<br />

A<br />

horizontal black dotted line was displayed in the center<br />

of the CRT, to serve as a target for the tracking task,<br />

A protective plastic cover was installed in front of the<br />

tube and on the face of the panei, to protect the subjects<br />

should any damage occur to the tube,<br />

Suitably located with respect to the field of<br />

vision, and immediately above the tube, two colored signal<br />

bulbs were mounted on the front panei,<br />

One of the bulbs,<br />

when lighted, was green indlcatlng that the subject should<br />

start working,<br />

The other, when lighted, gave a red signal<br />

indicating that the subject should stop,<br />

The two lights<br />

were activated by a switch located in the experimenter's


46<br />

station and within easy reach of the experimenter. Figure<br />

12 shows the mounted cathode ray tube and the signal lights,<br />

The signal switch is shown in Figure 13,<br />

One side of the Performance Console was cut out,<br />

to allow the subjects to get into the work station freely,<br />

The other side had a slot in which the hand rest and control<br />

assembly could slide freely upward and downward, for<br />

adjustment to the subject's height, On the left side of<br />

the console and within easy reach of the subject, a button<br />

for the control of vibration was installed should the subject<br />

have felt the need for stopping the experiment, Immediate<br />

stoppage of vibration by this means is a wise precautionary<br />

measure in such types of study, The emergency stop button<br />

is shown in Figure 9 (page 43),<br />

Hand Rest and Control Assembly Device<br />

A hand rest and control assembly device was constructed,<br />

providing several deslrable features: a control<br />

lever necessary to the tracking task; a place to rest the<br />

arm, thus preventing the subjects from leaning on the hand<br />

controller when fatigued during tasks of long duration; a<br />

design which forces ali subjects to assume the same posture<br />

in controlling the task; a construction which allows extra<br />

sensitivity and easier manipulation of the fingers in the<br />

tripodo grasp, which the subjects were instructed to use,<br />

The hand rest was a wood roller mounted on a<br />

bolt and moving freely around its axis, It was covered


47<br />

Fig. 12.^-Cathode ray tube ând signal<br />

lights<br />

Fig. 13.—Signal playing apparatjs, change of<br />

polarity circuit, vibration platform activator and<br />

signal switc^1,


with a foam rubber material, to provide a soft cushion for<br />

48<br />

the arm.<br />

The hand controller was an aluminum lever with a<br />

small rounded head, mounted on a potentiometer providing<br />

the voltage for the subject's output signal.<br />

Both hand<br />

rest and control device were mounted on one board, which<br />

slides freely on the side of the Performance Console and<br />

may be secured in any position by bolts and wing nuts.<br />

Figure 14 plctures the hand rest control assembly in position<br />

for instrument's calibration.<br />

Figure 15 shows the<br />

tripodo grasp used by the subjects.<br />

Seat<br />

The seat used in this experiment was a standard<br />

laboratory stool with a backrest.<br />

It was adjustable in<br />

height and position with respect to the work station.<br />

The<br />

seat was rigidly attached to the vibration platform and<br />

centered directly above the forcing function of the platform.<br />

No padding of any kind was used on it, nor were<br />

straps or harnesses provided.<br />

Figure 30 (page 85) shows<br />

the stool mounted on the platform.<br />

Signal Playing Apparatus<br />

The signal playing apparatus shown in Figure 13 (page<br />

47) consists of a regular sweep circuit for the horizontal<br />

sweep on the cathode ray tube.<br />

The vertical sweep on<br />

the CRT is controlled by the voltage output of the tape


49<br />

Fig. 14.—Hand rest and control assembly<br />

device<br />

Fig. 15.—Subject's controlling<br />

position


50<br />

recorder. This voltage output is rectified into a positive<br />

DC voltage when passed to the input of a vertical amplifier<br />

producing the vertical sweep on the CRT.<br />

The hand controller operated by subjects is connected<br />

to a potentiometer which produces a negative voltage counteracting<br />

the positive voltage obtained from the recorded signal,<br />

UJhen the signal was adjusted to the line in the middle of<br />

the CRT and the hand controller was centered in the vertical<br />

position, a negative voltage of 1.5 volts was introduced<br />

by the potentiometer.<br />

The voltage input from the recorded tape and the<br />

voltage output from the hand controller were subtracted in<br />

the circuit. The net voltage was then passed to the change<br />

of polarity circuit. A schematic diagram of the CRT sweep<br />

circuits and power supply is shown in Figure 16,<br />

Change of Polarity Circuit<br />

In order to convert the subject's error into an<br />

absolute error score, a change of polarity was required<br />

when the signal reversed its direction, This allowed integration<br />

of the signal over time, A special circuit (shown<br />

in Figure 17) was constructed for this purpose, A supply<br />

unit powered the change of polarity unit, and the potentiometer,<br />

as shown in the circuit.<br />

Analog<br />

Computer<br />

An analog computer of type PAGE TR-10, manufactured<br />

by Electronic Associates, Inc., New Jersey, was used to


52<br />

•H<br />

D<br />

ü<br />

M<br />

•H<br />

U<br />

(-1<br />

O<br />

CL<br />

U-<br />

O<br />

Q}<br />

cn<br />

c<br />

(TJ<br />

U<br />

o<br />

u<br />

•H<br />

-P<br />

(O<br />

E<br />

(D<br />

JI<br />

U<br />

tn<br />

I<br />

cn<br />

•H


53<br />

integrate the absolute error signal over a period of time<br />

(Figure 19).<br />

A schematic of the integrating circuit for the<br />

analog computer as used in this study is shown below.<br />

This<br />

integrating circuit provided the means for having a direct<br />

error score for the subject's performance.<br />

Output<br />

-0,5V, j^gj^<br />

—o 'VNA^<br />

O.Ov.<br />

I—A'<br />

(Absolute)<br />

+ 10<br />

0,5 Signal<br />

+0.5v<br />

Fig. 18.—Schematic of the analog computer integrating<br />

circuit.<br />

Dynagraph Recorder<br />

A Beckman Type R Dynagraph Recorder was used in this<br />

experiment to provide a means for measuring the error score.<br />

It was used, also, to monitor the experiment variables<br />

continuously.<br />

The input signal from the tape was recorded<br />

on channel number 2; the output signal from the hand controller,<br />

on channel number 1.<br />

The algebraic sum of the two<br />

signals was recorded on channel number 3.<br />

Channel 6 provided


Fig. 19.—View of the analog computer showing<br />

integrating circuit connections.<br />

54


55<br />

the recording of the integrated signal, displayed on channel<br />

3, over time. Channel 4 was connected to the accelerometer's<br />

switch to give an indication of the acceleration of tne<br />

switched on accelerometer.<br />

Fig. 20,—Dynagraph recorder


56<br />

Supporting Equipment for Controlling<br />

the Wariable<br />

Signal Recording Apparatus<br />

The signal recording apparatus was designed to give<br />

a complex profile signal which will repeat itself after a<br />

constant period of time,<br />

It consists of a cam which was<br />

designed to give an oddly shaped and complex signal,<br />

The<br />

cam was mounted on a disc driven by a variable speed motor<br />

through a pulley and V-belt,<br />

A rod through a roller camfollower<br />

connected it to a potentiometer,<br />

Rotation of the<br />

cam caused the follower to move in the same fashion as the<br />

cam profile,<br />

The potentiometer serves as a means of changing<br />

the amplitude of the constant áudio signal generated<br />

by the oscillator,<br />

The signal recording apparatus and<br />

supporting equipment are shown in Figures 21 and 22,<br />

UJide Range Oscillator<br />

A Hewlett-Packard Company ílflodel 2005D wide range<br />

oscillator was used to provide a constant audio-frequency<br />

of 1,000 cycles,<br />

The oscillator has special circuitry which<br />

ensures an output voltage of low distortion and high stability<br />

with any output load impedance from zero ohms to<br />

open circuits,<br />

A voltmeter was connected to the oscillator<br />

to provide a means of checking the quality of the signal input<br />

to the tape recorder,<br />

A voltage regulator was also used<br />

to prevent any voltage drop in the power line (Figure 23),


Fig, 21<br />

and voltometer. —Signal<br />

recording apparatus, oscillator<br />

Fig. 22.—Tape recorder, oscillator and voltmet er


zb<br />

Fig. 23.—Voltage regulator<br />

Fig, 24.—View of signal and vibration monitor-<br />

equipment.<br />

ma


ITIagnetic 'U'le<br />

Recorder<br />

59<br />

A mcdei 761 Ampex magnetic tape recorder/producer<br />

was used to record a complex signal for replaying on the CRT.<br />

This recorder/player<br />

features three heads; separate deep gap<br />

play/monitor; hea : for direct-monitor from the tape; soundwith-sound;<br />

sound-on-sound; and echo effect. A Scotch brand<br />

magnetic taoe of Dynarang Series 201 was used for recording<br />

and replaying the áudio signal, This type of tape was<br />

selected because of its low noise features which help to<br />

prevent áudio dropout,<br />

Earphones<br />

Standard type earphones were used to screen out<br />

ambient noise as well as noise of operation of the vibration<br />

platform,<br />

They had certain features by which each subject<br />

could adjust them correctly to his own head,<br />

(Tleasuremen t<br />

The most important measurement made in this investigation<br />

was that of the subJBct's performance.<br />

Vertical<br />

tracking ability was used as the performance criterion,<br />

The tracking apparatus, an assembly of the separate equipment<br />

parts mentioned earlier in this text, consists of a<br />

5-inch cathode ray tube<br />

(CRT), mounted in the center of a<br />

display console,<br />

A horizontal line, displayed at the center<br />

of the CRT, served as the target,<br />

The controlled element


60<br />

seen as a beam of light on the CRT (produced by the sweep<br />

circuit), is driven upward and downward by a program prerecorded<br />

on a magnetic tape,<br />

The subject's task was to<br />

maintain alignment of the controlled element with the horizontal<br />

line displayed in the center of the CRT, using a<br />

hand controller,<br />

The deviation of the controlled element from the<br />

center of the circle represents the sum of voltage inputs<br />

from the programmed tape, and voltage outputs generated by<br />

the subject's movement of the hand controller,<br />

This sum<br />

was then passed onto the change of polarity circuit to<br />

unify the sign of the voltage output and allow for recording<br />

an absolute error,<br />

This absolute error was then integrated<br />

by means of an analog computer over a period of 45<br />

seconds,<br />

The resulting value of integration was recorded<br />

on a dynagraph recorder and read as an error score in terms<br />

of the number of chart deviations on the recorder, i.e.,<br />

arbitrary units served as an error score.<br />

measure of performance in this experiment,<br />

This was the<br />

No effort was<br />

made to calibrate the recorder to read the exact voltage<br />

output because of its irrelevancy to the purpose of this<br />

study,<br />

The error score was continuously recorded while<br />

the subject was performing the task.


CHAPTER<br />

III<br />

EXPERIÍYIENTAL DESIGN<br />

This chapter is pertinent to three sectors of the<br />

experiment: the task, the variables and the design, The<br />

experimental routine is given, also,<br />

The<br />

Task<br />

j A compensatory one-dimensional vertical tracking<br />

task was utilized, The tracking system consisted of a<br />

visual display with two indications, one fixed (target),<br />

and the other moving (controlled element); a controlling<br />

device; and an operator to perform the tracking function,<br />

In compensatory tracking tasks, such as the one used in<br />

this study, the subject must manipulate the controlling<br />

device to superimpose the controlled element on the target,<br />

Any difference represents an error and the function of the<br />

operator is that of manipulating the controls to eliminate<br />

or minimize this error, In this study the CRT served as<br />

the visual display; the horizontal dotted black line in the<br />

center, the target; and a beam of light on the CRT, the<br />

controlled element, The latter was moved up and down by<br />

means of the electronic equipment prevlously described.<br />

61


62<br />

The human tracking function is a man-machine closed<br />

loop system,<br />

A closed loop system is one in which the output,<br />

or some result of the output is measured and fed back<br />

for comparison with the input (Childs, 1965).<br />

Figure 25 is<br />

an illustration of a tracking system.<br />

The signal input to<br />

the system is usually characterized by a ramp, step, sinusoidal<br />

or complex function, or a combination of these,<br />

The input signal used in this study was one of<br />

complex shape.<br />

It was recorded on a tape by means of a<br />

signal recording device and a cam possessing the same profile<br />

as the desired signal.<br />

Figure 26 shows the cam profile,<br />

and Figure 27 shows the signal input as recorded on a dynagraph<br />

recorder,<br />

This relatively complicated profile was<br />

selected for its ability to minimize the subject's adaptation<br />

to the tracking signal, )<br />

A tracking task was selected as a performance measuring<br />

task for several reasons,<br />

The tracking function is<br />

important in many military, industrial and Space situations,<br />

and tracking performance was shown to have suffered by<br />

vibration in many studies,<br />

In explaining the importance<br />

of the vibration effect on tracking performance and its<br />

incorporation in a system design situation, Chaney and<br />

Parks (1964) say:<br />

Definition of operator performance capability as<br />

influenced by system environmental conditions, is<br />

becoming incroasingly important as modern manned


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66<br />

systems become more complex. To the system designer,<br />

the accuracy and speed with which an operator can<br />

accomplish assigned visual-motor and tracking tasks<br />

within the operational environment is probably the<br />

largest contributing factor to the salection of a<br />

final display-control configuration,<br />

Vibration was proved to be the cause of decrements in<br />

tracking performance ability (Ashe, 1963; Gorrill and Snyder,<br />

1957; Catterson, 1962; Frazer, et ai., 1961; and others),<br />

In a paper<br />

(1962), Hornick concluded:<br />

UJhile there are discrepancies, there is general<br />

agreement that compensatory tracking ability shows<br />

a decrement which is related to amplitude and acceleration<br />

increases and vibration duration in the range of<br />

1 to 30 cps,<br />

In some experiments (Buckhout, 1964), vertical tracking<br />

error increased from 34 per cent to 74 per cent over the<br />

control trials,<br />

These are likely to be unsatisfactory leveis<br />

of decrement in an operational situation (Harris, et ai,,<br />

1965),<br />

The importance of the task and the detrimental<br />

effects of vibration upon its performance, made it challenging<br />

to investigate the effect of the latter in a prolonged<br />

period study, and totry to offer means of improving the<br />

performance during such a period,<br />

The Variables<br />

Independent Variables<br />

UJork/Rest Schedule, — The work/rest schedule as defined in<br />

this experiment differs slightly from the classical


67<br />

interpretation of it, although it conforms with the overall<br />

objectives of its utilization,<br />

íYlost of the research done<br />

regarding the effect of a work/rest schedule upon performance<br />

concentrated upon a duration of more than thirty hours,<br />

In<br />

their explanation of the importance of a work/rest schedule<br />

and its effect upon performance, Adams and Chiles (1963) wrote<br />

"A significant feature of many future man-machine systems is<br />

the extent to which they will depend upon efficient utilization<br />

of crew members."<br />

Adams and Chiles focused their<br />

efforts upon the long period missions.<br />

The efficient utilization of crew members is of<br />

great importance in ali criticai missions, especially those<br />

during which performance is influenced by some environmental<br />

factor, such as vibration, which imposes certain limitations<br />

upon intensity and exposure time for the subject,<br />

Scheduling<br />

the phases of work and rest under vibration in a certain way<br />

within the limits of safe exposure time may cause improvement<br />

in mission performance,<br />

Such questions, then, arise as these:<br />

Is there an optimum work/rest schedule which may be<br />

adapted for use under vibrational conditions?<br />

Does an interchange of the phases of work and rest<br />

allow.the subject to recover?<br />

If there is recovery, what is its nature in this<br />

case?<br />

lyiany others may be triggered,<br />

This study was designed<br />

to obtain answers to some of these many questions.


68<br />

j Four work/rest schedules were selected for testing<br />

during this research, "work" here referring<br />

to task performance,<br />

and "rest" referring to no task performance. The<br />

schedule's durations were selected within a simulated mission<br />

of one hour, where crew members are subjected to vibration<br />

throughout the mission period,<br />

The work/rest schedules were<br />

selected to provide the means to test if changing the schedule<br />

will affect the crew performance and consequently, the<br />

whole mission performance.<br />

They were selected in such a way,<br />

also, as to allow crew members<br />

(in a practlcal situation) to<br />

interchange work and rest periods if deslrable.<br />

The four<br />

work/rest schedules employed were divided into the following<br />

work periods:<br />

1. Thirty minutes of continuous work<br />

2. Two fifteen-minute periods of work<br />

3. Three ten-minute periods of work<br />

4. Six five-minute periods of work<br />

Figure 28 shows the work/rest schedules and their<br />

distribution throughout the mission duration. The total work<br />

and rest periods were determined in such a way that the work<br />

periods fell within the safe durations of exposure to long<br />

periods of vibration under the specified leveis of g in this<br />

experimen t.<br />

The Environment.—The experiment was performed under two<br />

environmental<br />

conditions:


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70<br />

1. Normal (nil-vibration)<br />

2. Vibration<br />

Selection of these two environments allowed detection<br />

of two performance effects:<br />

the task effect; the vibration<br />

effect.<br />

Performance in a normal environment was taken as<br />

a base levei with which performance under vibrational environment<br />

can be compared.<br />

Individuais were subjected to a levei<br />

of vibration of approximately 0.20 g.<br />

The frequency was set<br />

at 5 cps (body resonance frequency), with an amplitude of<br />

approximately 0.1 inch. )<br />

These leveis of frequency and amplitude were selected<br />

for several reasons.<br />

The low levei of frequency was selected<br />

because vibrational research is focused upon the low frequency<br />

range.<br />

(Ylagid, Ziegenruecker and Coermann (1960) employed a<br />

low frequency range of 1 to 20 cps to investigate human tolerance<br />

of vibration,<br />

They justified this as follows:<br />

(1) Buffeting and impact loads as they occur in<br />

Space vehicles and in high speed, low altitude flights,<br />

have a frequency spectrum of this range , , ,; (2)<br />

resonances of important body áreas were found within<br />

this range , , ,; (3) pilots can easily be protected<br />

against frequencies above 20 cps by mechanical damping<br />

systems.<br />

Harris supported this view and wrote (1965):<br />

In my opinion our greatest need for behavioral<br />

studies is in the low g range within the frequencies<br />

of 1 to 20 cps. I believe it is necessary that we<br />

systematically study performance changes within this<br />

range. From such studies we would hope to be able to<br />

specify for a given frequency at what intensity levei<br />

Gignificant decrement begins to occur.


71<br />

Chaney and Parks (1964) write:<br />

Low frequency vibration is an important part<br />

of many operational environments and is perhaps the<br />

most difficult to design out of the system. Consequently,<br />

a criticai need exists for data concernlng<br />

vibration effects on human ability to perform perceptual<br />

and motor control activities, and design<br />

features which will enhance their accomplishment.<br />

(ílost vehicles, moreover, produce vibrations of<br />

frequencies ranging from 1 to less than 10 cps (Figure 1,<br />

page 9).<br />

The higher frequencies are easily and generally<br />

attenuated (Radke, 1957).<br />

In a paper by Harris (1965), he compared the results<br />

of several studies on tracking performance.<br />

He then composited<br />

the curve shown in Figure 29.<br />

The geometric symbols<br />

in the figure refer to the studies of particular authors.<br />

Their locations on the figure indicate the leveis of vibration<br />

at which the tracking function was tested.<br />

The numbers<br />

inside the symbols show the relative levei of decrement<br />

obtained within any one study.<br />

Number 1 denotes the greatest<br />

decrement, with successive numbers indicating decrecsing<br />

decrement.<br />

The absence of a number means that no decrement<br />

was obtained.<br />

Although conditions under which the experiments were<br />

pursued differed greatly, the leveis at which tracking decrements<br />

begin are still apparent.<br />

The greatest decrements in performance in general<br />

appear to be around 4-5 cps (body resonance): P cps and 11<br />

cps (resonance frequency of the facial musculature).<br />

The


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FREQUENCY (CPS)<br />

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berge?"^g65) '^^°'^'^^^^^d limits, (From Harris anu Shoen-


decrements occurring under 8 and 11 cps, however, were under<br />

73<br />

a higher g levei than those occurring at 5 cps,<br />

These<br />

results, in addition to the helplessness of the body to<br />

avoid the criticality of its resonant frequency<br />

(5 cps),<br />

made this 5 cps levei the most deslrable one with which to<br />

work,<br />

It has been argued that tracking decrement is related<br />

primarily to amplitude of vibration, modified by a<br />

fractional component of frequency, Catterson, et ai,, (1962)<br />

suggested that regardless of differences in frequency, the<br />

most significant deterioration occurred in association with<br />

the change in amplitude of the vibration.<br />

For this study<br />

it was necessary to select a levei of acceleration failing<br />

within the maximum tolerance levei of one hour or less of<br />

vibration exposure,<br />

It is to be noted that the levei of<br />

g selected was 0,20, which does fali within the tolerance<br />

limit to vibration of one hour or less given by Linder (1962),<br />

and slightly higher than the one suggested by Harris (1965),<br />

The frequency levei of 5 cps, and the amplitude of 0,08<br />

inches, fali within the low frequency, high amplitude category,<br />

and for most practlcal purposes, according to previous<br />

tracking studies may produce certain performance effects,<br />

allowing sensitive detection of variables.<br />

Several investigators used comparative leveis of<br />

frequency and amplitude,<br />

Frazer, et ai., (1961) exposed<br />

their subjects to frequencies of 2, 4, "^ and 12 CPS, and


74<br />

double amplitudes of 0.063, 0.125, 0,189 and 0,250,<br />

Simmons<br />

and Hornick (1962), used frequencies of 1.5, 2,5, 3.5, 4,5<br />

and 5,5 cps and g leveis of ,15, ,25 and 0.3,<br />

their subjects to vibration for thirty minutes,<br />

They exposed<br />

Other<br />

investigators used similar leveis,<br />

Dennis (1960), in an experiment of visual acuity,<br />

held a peak acceleration constant and varied the frequency,<br />

The greatest error occurred at 5 cps at ,25 g, and at 14 cps<br />

when acceleration was maintained at ,5 g,<br />

The Period,—Each schedule was divided into nine performance<br />

periods, six periods failing within the controlled environment<br />

span of time (normal and vibrational), the other within<br />

the recovery span, as illustrated in Figure 28 (page 69),<br />

A performance period is five minutes long, with a performance<br />

score based upon the integrated error of subject's tracking<br />

over forty-five seconds of every one minute of work,<br />

Subjects<br />

worked in multiples of whole periods (multiples of five<br />

minutes) during the controlled environment span, and for a<br />

one minute interval,' only, at the beginning of each recovery<br />

period.<br />

Periods were selected as a variable because of the<br />

importance of analyzing performance with respect to time of<br />

exposure,<br />

lYlost of the previous studies focused upon short<br />

time periods (less than thirty minutes), and investigators<br />

in general did not attempt to analyze performance with respect<br />

to duration of time of exposure.


75<br />

In support of this point, Harris and Chiles (1964)<br />

wrote:<br />

, , , several important variables have not received<br />

sufficient attention in vibration research, One of<br />

these variables is the duration of exposure period,<br />

In the typical vibration study involving a tracking<br />

task, a fixed duration is selected for investigation,<br />

and the performance data are (perhaps) broken down<br />

into first half versus second half.<br />

ílflon itor ing performance continuously over the working<br />

period, as was done in this experiment, was not a usual<br />

procedure in preceding experiments.<br />

Investigators used,<br />

rather, only a sample of performance at different points<br />

in their experiments (Catterson, et ai., 1962; Holland, 1967;<br />

and others).<br />

The one minute of work during recovery periods in<br />

this study was required to ootain error scores during the<br />

span of recovery specified.<br />

The Dependent Variables<br />

The dependent variables discusser! here include:<br />

1. lYleasured dependent variables<br />

2. Calculated dependent variables<br />

ÍYleasured Dependent 'iariablíps. — The measurer! dependent<br />

variable used in this study was the absolute error score<br />

resulting from performance of a vertical r.rficking task and<br />

integrated over the first forty-five secoids of eacn mmute<br />

of<br />

work.


76<br />

The difference between the input signal from the<br />

program displayed on the cathode ray tube, and the output<br />

signal from the potentiometer connected to the hand controller<br />

and monitored by the subjects, were added absolutely<br />

(in terms of voltage), using the electronic equipment<br />

described in Chapter II.<br />

This value was then integrated<br />

over time, by means of the analog computer.<br />

A continuous<br />

record of the input signal, the output signal, the difference<br />

and the integrated value was obtained with the Dynagraph<br />

recorder,<br />

The error score was read in terms of chart divisions<br />

on the recorder (arbitrary units).<br />

Figure 27 (page<br />

65) shows a complete chart recording of an actual run under<br />

vibration,<br />

Calculated Dependent Variables,—The two calculated dependent<br />

variables used in this study were the difference in average<br />

error score for perfoimance under vibration and performance<br />

in a normal controlled environment for the particular work/<br />

rest cycle used; and the average percentage of increase in<br />

error for performance under vibration,<br />

In order to test for only the effect of vibrational<br />

stress on performance, it was assumed that the subject's<br />

performance under normal environment represents his proficiency<br />

in tracking at the levei of the work/rest schedule<br />

used,<br />

This is considered a rear^onable assumption, since<br />

subjects' leveis of performance were raised before the


77<br />

actual start of the experiment until they leveled off.<br />

Ali<br />

of the experiments were run in a random fashion.<br />

The error<br />

score readings over each five-minute work period were averaged<br />

for normal and vibrational environments,<br />

The difference<br />

between average error reading of work under vibration, and<br />

the average error during nil-vibration<br />

(normal environment),<br />

was then taken as the net average error score for the individual<br />

subject at that particular levei of the work/rest<br />

schedule,<br />

This was used as a dependent variable in an<br />

analysis of variance, as will be discussed later in this<br />

chapter.<br />

The second calculated dependent variable, the percentage<br />

of increase in average error score, was calculated<br />

as follows:<br />

Percentage of increase in error =<br />

Average vibration error -<br />

average nil vibration error<br />

Average nil vioration error<br />

The average error is once more an average of the<br />

five-minute readings taken within each period.<br />

This dependent<br />

variable was used in another ANOVA, as indicated later<br />

in this chapter.<br />

The Controlled Variables<br />

Signal Input.—The signal input was in the form cf<br />

a complex<br />

function.<br />

To record it, a cam possessinr, the sane profile<br />

as the required signal was used, and procedures prevlously<br />

discussed were followed.


78<br />

The reason for chooslng a complex profile signal<br />

was to decrease the amount of the subjects' ndaptation to<br />

the signal pattern.<br />

Repetition of the signal profile provided<br />

the means of comparing performance directly from<br />

output.<br />

Normal Environment,—A normal environment was controlled<br />

here by establishing a nil-vibration situation.<br />

In the<br />

meantime, subjects plugged their ears with cotton and<br />

wore headphones to prevent the ambient noise from affecting<br />

performance,<br />

The room temperatura was kept constant at<br />

72° F i 1° throughout the performance, The light intensity<br />

was kept constant, as well.<br />

Vibrational Environment,—A frequency of 5 cps was the<br />

vibrational levei maintained for this experiment, uith an<br />

amplitude of 0,08,<br />

To calculate the g levei for this combination<br />

of frequency and amplitude the following formula is<br />

used (Harris, et ai,, 1965):<br />

g = 0.0511 AF2<br />

where:<br />

g = peak acceleration in terms of the<br />

acceleration of gravity<br />

A = double amplitude (DA) in inches<br />

f = frequency cps<br />

The g levei selected for this experiment uas approximately<br />

0,20 g at 5 cps, which gives the above values of<br />

amplitude.


79<br />

In the literature performance was shown to be<br />

most affected by vertical vibration,<br />

This was especially<br />

true in the case of tracking performance, and was the reason<br />

for selecting vertical vibration as the controlled environment<br />

for this study,<br />

Since most of the previous research<br />

on vibration had been done under conditions of sinusoidal<br />

vibration, it was decided to employ it for this research,<br />

in order to make use of the findings of some other investigators.<br />

It was argued, however, that there is no significant<br />

difference in performance between random and sinusoidal<br />

vibration (UJeisz, et ai,, 1965), and that in basic research<br />

(such as this) sinusoidal vibration may be used and then<br />

followed by other types of vibration in future research<br />

(Johnston, 1969),<br />

The leveis of frequency and acceleration used in<br />

this study were monitored by means of accelerometers throughout<br />

the experiment,<br />

Appendix B gives the value of g<br />

calculated from the accelerometer outputs.<br />

Statistical Design of the Experiment<br />

Three analyses of variance were run to allow testing<br />

of the desired variables,<br />

These analyses and the models for<br />

each are given below:<br />

First Analysis of Variance<br />

The three independent variables, work/rest schediies.


80<br />

environments and periods are analyzed in order to determine<br />

their effects upon the dependent variable; namely, tracking<br />

performance in terms of absolute error score during the<br />

first minute of each period,<br />

Analysis of variance was based upon mixed model<br />

techniques,<br />

A completely randomized factorial model 7 x 4 x<br />

2x9 fits this experiment. To obtain the most Information<br />

out of the design, however, the experiment was run in a<br />

randomized block factorial design, with subjects (7 leveis)<br />

serving as blocks,<br />

This heips to block out individual differences<br />

between subjects,<br />

A summary of factors used is<br />

given in Table 1,<br />

TABLE 1<br />

SUiniyiARY OF FACTORS<br />

Factor Label Levei Type Effect<br />

Subjects<br />

S<br />

UJork-rest schedule UJ<br />

Environmen t<br />

Period<br />

V<br />

P<br />

1 30 min,<br />

2 2/15 min,<br />

3 3/10 min,<br />

4 6/5 min.<br />

1 normal<br />

2 vibration<br />

1<br />

2<br />

3<br />

4<br />

5<br />

6<br />

7<br />

8<br />

9<br />

Random (Blocks)<br />

Fixed<br />

Fixed<br />

Fixed


The model for the randomized block desjgn which<br />

81<br />

was used (Hicks, 1966) is as follows:<br />

X = U 4- A(I) + B(J) + AB(IJ) + C(K) + AC(JK) -f-<br />

BC(JK) + ABC(IJK) -f 5(L) -f E(lJKL)<br />

where<br />

X =<br />

dependent variable observed at I, J, K, L<br />

u<br />

A(I)<br />

B(J)<br />

C(K)<br />

S(L)<br />

I<br />

J<br />

K<br />

L<br />

E(IJKL)<br />

of their respective treatment<br />

= common effect of the whole experiment<br />

= first factor effect (work/rest schedule)<br />

= second factor effect (environment)<br />

= third factor effect (period)<br />

= replications (blocks)<br />

= 1, 2, 3, 4<br />

= 1, 2<br />

= 1, 2 , , , 9<br />

= 1, 2 , , , 7<br />

= error term (random)<br />

A completely randomized order for the different leveis<br />

within blocks was used,<br />

Table 2 shows the design for the<br />

estimated mean square (EíílS) and the ratios required for the<br />

F-statistic.<br />

Second Analysis of Variance<br />

The two dependent variables, work/rest schedule and<br />

period, are analyzed to determine their effects jpon perforf..anc'''<br />

under a vibratioril environment,<br />

The dependent


82<br />

variable was the difference between the average error score<br />

under vibration and that under nil-vibration (normal environment),<br />

The model was a randomized block factorial design<br />

embodying four leveis of work/rest schedules, periods and<br />

seven replications (blocks), This model is given by<br />

X = U -f A(I) + C(K) + AC(IK) + 5(L) +<br />

E(IKL)<br />

TABLE 2<br />

EXPECTED (YIEAN SQUARE FOR EXPERIÍYIENTAL<br />

DESIGN<br />

df<br />

(Ylodel<br />

4<br />

F<br />

I<br />

2<br />

F<br />

J<br />

9<br />

F<br />

K<br />

7<br />

R<br />

L<br />

EIYIS<br />

F<br />

Test<br />

3<br />

1<br />

3<br />

8<br />

24<br />

A(I)<br />

B(3)<br />

AB(IJ)<br />

C(K)<br />

AC(IK)<br />

0<br />

4<br />

0<br />

4<br />

0<br />

2<br />

0<br />

0<br />

2<br />

2<br />

9<br />

9<br />

9<br />

0<br />

0<br />

7<br />

7<br />

7<br />

7<br />

7<br />

2<br />

^e<br />

2<br />

^e<br />

2<br />

^e<br />

2<br />

^e<br />

4<br />

+<br />

+<br />

+<br />

+<br />

+<br />

126<br />

252<br />

63<br />

56<br />

14<br />

2<br />

^A<br />

2<br />

^B<br />

^AB<br />

^l<br />

^AC<br />

A/e<br />

B/e<br />

AB/e<br />

C/e<br />

AC/e<br />

8<br />

BC(JK)<br />

4<br />

0<br />

0<br />

7<br />

<<br />

-f-<br />

28<br />

^§C<br />

BC/e<br />

24<br />

ABC(IJK)<br />

0<br />

0<br />

0<br />

7<br />

a2<br />

e<br />

+<br />

7<br />

a2<br />

ABC<br />

ABC/e<br />

4 26<br />

E(IJKL)<br />

1<br />

1<br />

1<br />

1<br />

a2<br />

e<br />

—<br />

503


Third Analysis of Variance<br />

83<br />

The analysis of variance in the above experiment<br />

covers both the performance and recovery periods.<br />

In order<br />

to analyze the results during the vibration period alone,<br />

another analysis of variance was run.<br />

The results covered<br />

the first six periods of performance only, i.e., during the<br />

vibration periods, but eliminating the recovery periods,<br />

Again, the analysis for this experiment was a randomized<br />

block factorial design, with 4x6<br />

leveis and seven replications<br />

(blocks),<br />

The model is as given before in the<br />

section regarding the second analysis of varirince experiment,<br />

The dependent variables were the differences in average<br />

error score under conditions of vibration and nil-vibration,<br />

and the percentage of increase in average error score over<br />

the five-minute period of work under conditions of vibration.<br />

Subjects<br />

Soven maie undergraduate students served as subjects<br />

in this experiment,<br />

Five of those had prevlously particlpated<br />

in other intra-departmental studies of vibration.<br />

To the other two, vibrational study was a new experience.<br />

Ali subjects had undergone thorough physical examinations,<br />

and had proved to be in excellent health,<br />

Table 3 is a<br />

summary of the Information obtained from subjects.


84<br />

TABLE 3<br />

SUBJECT<br />

INFORÍYIATION<br />

Subject<br />

Number Age Classif ication Height UJeight Handedness<br />

1, Valusek 21<br />

Júnior<br />

6'1"<br />

165<br />

Right<br />

2, Stafford 24<br />

Sênior<br />

6'<br />

170<br />

Right<br />

3, UJarren 22<br />

Sen ^or<br />

6»<br />

165<br />

Right<br />

4, Ness 24<br />

Sênior<br />

6'<br />

175<br />

Right<br />

5, UJideman 20<br />

Júnior<br />

6'<br />

170<br />

Right<br />

6, Visser 21<br />

Júnior<br />

5'<br />

165<br />

Right<br />

7, 0'Brien 21<br />

Júnior<br />

5'lOè"<br />

151<br />

Right<br />

Experimental Routine<br />

( The experiment was conducted in the new vibration<br />

laboratory located on the first floor of the Industrial<br />

Engineering Buildlng at Texas Tech,<br />

The room is airconditioned<br />

and basically a constant temperature was kept<br />

.throughout the experiment,<br />

Before beginning, the subjects were brought to the<br />

laboratory for briefing,<br />

They were informed of the exact<br />

requirements from each, and given a description of the method<br />

of conducting the experiment, as well as of the task to be<br />

erformed.


85<br />

Fig. 30.—Vibration<br />

facility


86<br />

After checking on the subjects' health, background<br />

and the results of their physical examinatlon, an experiment<br />

schedule was made for each to suit his convenience, «The<br />

first sessions were devoted to acquainting the subjects with<br />

the equipment and procedures, and in answering any questions<br />

they might have,<br />

The following two sessions were devoted<br />

to raising the levei of performance of the subjects, until<br />

it started leveling off,<br />

This was done to avoid any learning<br />

effect of the task. j UJhen it was believed that the performance<br />

of a subject was still improving, an extra learning<br />

session was added,<br />

An example of a subject's learning curve<br />

is given in Appendix C,<br />

( After learning sessions were finished, actual experimentation<br />

sessions began,<br />

Upon arrival for each session,<br />

the subject was seated in a comfortable chair for five to<br />

ten minutes, a random draw for the experiment leveis at which<br />

he was to perform was made,<br />

The subject was informed of these<br />

leveis, and instructed to proceed to the experimental apparatus,<br />

where he was seated on the chair mounted on the platform.<br />

The accelerometers were then attached to his hip and head, and<br />

to the vibration platform.<br />

He was given a small piece of<br />

cotton with which to plug his ears as an extra defense against<br />

noise, and was instructed to wear the earphones.<br />

Ali of the<br />

electronic equipment was then switched on, and the experiment<br />

was continued as scheduled.)


87<br />

The experiment began with calibration of the equipment.<br />

The hand controller was brought to its central vertical<br />

position, and a signal of constant value was played by<br />

the recorder. The analog's potentiometers were then adjusted<br />

to give a zero integration value as long as the line was<br />

kept on<br />

target.<br />

For experimentation with a vibrational environment,<br />

the vibration platform was activated. A check was made on<br />

the accelerometer outputs. For performance of an experiment<br />

in a normal environment, the accelerometer power supply was<br />

not activated. UJhen it was the time scheduled for work to<br />

begin, the recorder was started, and the green command<br />

light in front of the subject*s eyes was switched on, signaling<br />

that he should begin performing the task.<br />

It is worthy of mention here that a short tone was<br />

recorded on the second channel of the tape recorder as an<br />

auditory signal to the experimenter at the beginning and<br />

end of each performance measuring interval (based upon 45<br />

seconds of integration for each one minute of work), UJhen<br />

this tone is first heard by the experimenter, the analog<br />

computer switch is turned to operate position and the integration<br />

process started, UJhen the second tone is heard,<br />

the computer switch is turned to hold, then reset, An<br />

error score on the dynagraph recorder chart is then read<br />

and<br />

recorded.


88<br />

r Continuous readings were taken for the subject's<br />

performance.<br />

A large clock was used to check the time<br />

periods throughout the experiment,<br />

At the end of each working<br />

period, the red signal command switch was turned on,<br />

and the tape recorder stopped,<br />

This procedure was repeated<br />

through ali work/rest schedules and with ali subjects,<br />

At<br />

the end of the one-hour period specified for the mission,<br />

and following the last period of work, the subjects continued<br />

working for one more minute and an error score was<br />

recorded,<br />

This reading was taken to check for recovery<br />

immediately following exposure,<br />

Two four-minute periods of<br />

rest, followed by one minute of work, completed investigation<br />

of the recovery period,<br />

The schedule of work, rest<br />

and recovery phases under normal and vibrational environments<br />

according to which the experiments were conducted<br />

is shown in Figure 28 (page 69),<br />

After the cessation of vibration, the subject was<br />

questioned regarding his reaction to its effect,<br />

Following the work/rest schedule (performance period)<br />

and the recovery period, the electronic equipment was<br />

switched off, and the accelerometers were removed from<br />

the subject's body and the vibration platform, the run<br />

being complete for that particular date,'<br />

Safety Precautions<br />

Ali of the subjects were given a thorough physical<br />

examinatlon<br />

(the Tilaster Test) to ensure their physical


89<br />

Fig. 31.—SubjBct's station<br />

Fig. 32.—Experimenter station


90<br />

ability to particlpate in the experiment.<br />

The acceleration<br />

levei used in this experiment was within the tolerance limits<br />

established by Linder (1962) for exposure time of one hour<br />

or less.<br />

The acceleration intensity was monitored at the<br />

platform, hip and head, to ensure reasonable leveis of<br />

acceleration being transmitted to those locations,<br />

The g<br />

levei was calculated at each place,<br />

Pieces of cotton and a<br />

set of earphones were provided in order to screen out vibration<br />

platform and ambient noise, to eliminate any side effects<br />

these might have on performance,<br />

An emergency button to stop<br />

vibration was installed in the performance console, within<br />

easy reach of the subjects,<br />

They were instructed that should<br />

they have any feeling of pain, extreme discomfort, náusea<br />

or any other intolerable reaction, they should push the<br />

emergency stop button at once,<br />

They were under continuous<br />

observation, also, by the experimenter, for the purpose of<br />

keeping informed of their condition,<br />

It is worthy of mention<br />

that ali subjects completed ali experiments without having<br />

to stop the vibration.


CHAPTER IV<br />

FINDINGS AND IN TER PRETAT IONS<br />

The statistical technique of analysis of variance<br />

was employed in this study to determine the effects of<br />

the independent variables, namely work/rest schedules,<br />

environments and periods, upon the dependent variables<br />

prevlously defined,<br />

The F-statistic was used to test for<br />

the significant effects,<br />

Slgnificance was ascertained<br />

at the conventional leveis of one and five per cent,<br />

In order to thoroughly analyze the results obtained<br />

from this experiment, it was necessary to run three different<br />

analyses of variance,<br />

A randomized block factorial<br />

design was used in ali three ANOVA'S,<br />

This design helps<br />

block the subject effects, allowing a true testing of the<br />

variables,<br />

The ANOVA comoutations were performed on an<br />

IBlYI-360 computer using the program QADTANOVA, written by<br />

Charles Burdsal, Jr,<br />

The Texas Tech Statistical Library<br />

number of the program is TTS 050,<br />

The program provided<br />

the following Information:<br />

1, Source table for each independent variable<br />

2, F-ratio for ali main effects and interactions<br />

3, Exact probability of occurrence by cnance<br />

for ali main effects and interactions<br />

91


92<br />

4, Cell means for ali main eftects and interactions<br />

and their leveis of slgnificance,<br />

if any.<br />

Following the analysis of data, Duncan (Ylultiple<br />

Range Tests were performed to determine the significant<br />

differences between treatments.<br />

The results of the analyses<br />

of variance experiments performed and those obtained<br />

from the múltiplo range tests are discussed below,<br />

First Analysis of Variance Results<br />

The first analysis of variance was designed to<br />

test the hypotheses that work/rest schedules, environment,<br />

period, and their interactiuns, affect the absolute error<br />

score measured at the first minute of each performance<br />

period, The results of this ANOVA are shown in Table 4,<br />

As indicated in Table 4 environment had a highly<br />

significant effect upon human tracking performance.<br />

Table<br />

5 gives the cell means and standard deviation of this significant<br />

factor:<br />

environment,<br />

An increase in vertical tracking error of approximately<br />

43 per cent was noted when vertical vioration was<br />

introduced,<br />

This finding is in agreement with results<br />

obtained in other investigations of performance during a<br />

tracking task under a vibrational environment (Buckhout,<br />

1964, Harris and Shoenberger, 1965, Chaney and Parks, 1964,<br />

and others),<br />

The controlled v.Lbrational environment leveis


93<br />

in this experiment were selected in such a way as to fali<br />

within the region of performance decrement specified by<br />

other studies,<br />

Obtaining such a high performance decrement<br />

(43 per cent) indicates reasonable task difficulty, a<br />

necessary condition for providing a good measure of other<br />

variables of interest:<br />

the work/rest schedule and oeriod,<br />

A plot of means of absolute error score versus environment<br />

is shown in Figure 33,<br />

TABLE 4<br />

ANOVA FOR ABSOLUTE ERROR SCORE (NORIYIAL<br />

AND VIBRATIONAL EN V IRONÍÍlEN T)<br />

Source<br />

DF<br />

Sum of<br />

Squares<br />

í^lean<br />

Square<br />

F-Ratio<br />

Blocks<br />

6<br />

942.95<br />

157.16<br />

31.73*<br />

A, UJork/Rest<br />

3<br />

16,04<br />

5.35<br />

1.08<br />

B, Environment<br />

1<br />

1111,02<br />

1111,02<br />

224.67*<br />

AB<br />

3<br />

15,66<br />

5.22<br />

1,06<br />

C, Period<br />

8<br />

86,74<br />

10.84<br />

2,19*»<br />

AC<br />

24<br />

186,46<br />

7.77<br />

1.57**<br />

BC<br />

8<br />

50,93<br />

6.37<br />

1.29<br />

ABC<br />

24<br />

43,32<br />

1,80<br />

0.37<br />

Error<br />

426<br />

2105.60<br />

4. 35<br />

Total<br />

503<br />

4559.72<br />

• Signifijant at 1^ levei<br />

*• Significant at 5% levei


94<br />

TABLE 5<br />

lYlEANS AND STANDARD DEVIATION OF ENVIRONMENT<br />

EFFECT ON ABSOLUTE ERROR SCORE (NOR.TÍIAL<br />

AND VIBRATIONAL LN V IRONÍÍlEN TS )<br />

Environment lYlean Standard Deviation<br />

Normal<br />

Vibration<br />

6.93<br />

9.90<br />

2,39<br />

2,93<br />

The analysis of variance results also yielded a<br />

significant effect at the five per cent levei, for the<br />

period of performance,<br />

Table 6 gives the cell means and<br />

standard deviations of this significant factor. Figure 34<br />

is a plot of these means against the absolute error score,<br />

TABLE 6<br />

(YlEANS AND STANDARD DEVIATIONS OF PERIOD EFFECT<br />

ON ABSOLUTE ERROR SCORE (NORIYIAL<br />

AND VIBRATIONAL EN V IRONIYIEN T)<br />

Period<br />

fYlean<br />

Standard<br />

Deviation<br />

1<br />

2<br />

3<br />

4<br />

5<br />

6<br />

7<br />

8<br />

9<br />

8,44<br />

8,31<br />

9.11<br />

8.64<br />

8,80<br />

8,17<br />

7.53<br />

B.43<br />

8.30<br />

3.01<br />

3.07<br />

3,28<br />

3,44<br />

3,03<br />

2,93<br />

2.69<br />

2,70<br />

2,80


95<br />

10<br />

r<br />

CD<br />

M<br />

O<br />

U<br />

(/)<br />

U<br />

o<br />

u<br />

LiJ<br />

c<br />

CO<br />

CD<br />

CO<br />

-P<br />

•H<br />

C<br />

ZD<br />

>><br />

U<br />

CO<br />

Ul<br />

-p<br />

•H<br />

n<br />

u<br />

cc<br />

8<br />

Normal<br />

Vibration<br />

Environmen t<br />

^<br />

Fig. 33,—Plot of means of absolute error score<br />

versus environment.


96<br />

10<br />

CD<br />

Ul<br />

o<br />

cn to<br />

Ul<br />

o<br />

Ul<br />

Ul<br />

(D<br />

-P<br />

D<br />

—t<br />

o<br />

CO<br />

n<br />

-p<br />

•H<br />

c<br />

ZD<br />

>><br />

Ul<br />

CO<br />

Ul<br />

-p<br />

•H<br />

JD<br />

Ul<br />

8<br />

j _<br />

2 3 4 5 6 7 0 9<br />

Performance<br />

Recovery<br />

Period<br />

Fig, 34,—Plot of means of absolute error score<br />

versus period.


97<br />

The absolute error under controlled<br />

environments<br />

(normal and vibrational), stayed generally constant during<br />

the first two periods of performance, increased during the<br />

third, fourth and fifth periods, Significant improvement<br />

in performance occurred immediately following exposure<br />

(period 7).<br />

The error score increased agiin in the second<br />

and third periods of recovery (periods 8 .ri 9). An unexpected<br />

improvomont<br />

in performance duri ig :l e last period<br />

of exposure (period 6) may be noted from t le curve. An<br />

explanation o^ the behavior of this point ii delayed to a<br />

later section in .his chapter.<br />

The work/rest schedule, by period<br />

interaction,<br />

affected the absolute error score significantly at the five<br />

per cent levei.<br />

Figure 35 is a plot of the means of these<br />

interactions against the absolute error score. Table 7<br />

provides these means, as well as the standard devintions.<br />

In order to clarify the trends in this figure, a<br />

separate plot is given for each work/rest schedule uòed<br />

(Figures 36, 37, 38, and 39).<br />

UJhen the subjects performed<br />

in accordance with the first work/rest schedule, their error<br />

started high, tended to decrease in the middle of the run,<br />

and fluctuated up and down toward the end.<br />

UJhen the subjects performed in accordance with the<br />

second work/rest schedule, their error started hjgh, improved<br />

in the following period, then went up again in the third<br />

period.<br />

The same cycle was repeated in the second phase of<br />

work.


98<br />

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99<br />

TABLE 7<br />

ÍYIEANS AND STANDARD DEVIATION OF UJORK/REST BY<br />

PERIOD INTERACTION EFFECT ü^ ERROR SCORE<br />

(NORIYIAL AND VIBRATIONAL EN V IRONIYIEN T)<br />

UJork/Rest<br />

Period<br />

ÍYlean<br />

Standard<br />

Deviation<br />

1<br />

2<br />

3<br />

4<br />

1<br />

2<br />

3<br />

4<br />

1<br />

2<br />

3<br />

4<br />

1<br />

2<br />

3<br />

4<br />

1<br />

2<br />

3<br />

4<br />

1<br />

2<br />

3<br />

4<br />

1<br />

2<br />

3<br />

4<br />

1<br />

2<br />

3<br />

4<br />

1<br />

2<br />

3<br />

4<br />

1<br />

1<br />

1<br />

1<br />

2<br />

2<br />

2<br />

2<br />

3<br />

3<br />

3<br />

3<br />

4<br />

4<br />

4<br />

4<br />

5<br />

5<br />

5<br />

5<br />

6<br />

6<br />

6<br />

6<br />

7<br />

7<br />

7<br />

7<br />

8<br />

8<br />

8<br />

8<br />

9<br />

9<br />

9<br />

9<br />

8.63<br />

9,32<br />

8.25<br />

7.56<br />

8,3<br />

7,85<br />

7,74<br />

9,36<br />

8,08<br />

9.09<br />

9,79<br />

9,50<br />

7,99<br />

9,06<br />

7,73<br />

9,80<br />

8,46<br />

7,49<br />

9,88<br />

9,36<br />

7,92<br />

8,71<br />

7.34<br />

8,71<br />

7,36<br />

7,71<br />

8.01<br />

7.05<br />

7.90<br />

9.04<br />

8,77<br />

8,03<br />

8,36<br />

8.47<br />

8.73<br />

7.63<br />

3,04<br />

2,82<br />

3,55<br />

2,63<br />

2,94<br />

1,96<br />

3,59<br />

3.58<br />

2.80<br />

2,81<br />

3.86<br />

3.69<br />

3.50<br />

2.72<br />

2.86<br />

4.38<br />

2.79<br />

2.51<br />

3.32<br />

3.09<br />

3.10<br />

2.59<br />

3.53<br />

2.47<br />

2.73<br />

2,35<br />

3,34<br />

2.43<br />

2,16<br />

2,56<br />

3,09<br />

3.05<br />

2,90<br />

2.68<br />

3.18<br />

2.61


IGO<br />

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8<br />

z/<br />

/<br />

3 4 í<br />

Performance<br />

o - â — ^<br />

Recovery<br />

Period<br />

Fig. 36.—Plot of means of absolute error score<br />

versus period—UJ/R schedule I,


101<br />

10<br />

Q)<br />

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8<br />

j . X X<br />

2 3 4<br />

Performance<br />

Period<br />

8 9<br />

Recovery<br />

Fig, 37.—Plot of means of absolute error score<br />

versus period—UJ/R schedule II,


102<br />

10 .<br />

CD<br />

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cn<br />

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PorformancB<br />

Period<br />

7 8 9<br />

Recovery<br />

Fig, 38,—Plot of means of absolute error score versus<br />

period—UJ/R schedule III,


103<br />

10<br />

CD<br />

P<br />

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Performance<br />

Period<br />

8 9<br />

Recovery<br />

Fig. 39.—Plot of means of absolute error score versus<br />

period—UJ/R schedule IV.


Ulhen the subjects performed in accordance with the<br />

third work/rest schedule, their error score started high,<br />

104<br />

and improved in the following period,<br />

The cycle repeated<br />

itself twice more in this schedule for the second and third<br />

phases of work,<br />

UJhen the subjects performed in accordance with<br />

the fourth work/rest schedule, their error score stayed<br />

within a naorow range, except during the first period,<br />

when the error score was low,<br />

It is notable that under ali work/rest schedules,<br />

subjects' error scores decreased significantly immediately<br />

following the ends of the performance periods (start of<br />

recovery), then went up in the following periods of recovery.<br />

As shown from the above discussion, the results of<br />

the first analysis of variance indicated the validity of<br />

the hypothesis that environment, period and work/rest<br />

schedule by period interaction have a significant effect<br />

on the absolute error score,<br />

The hypothesis concernlng<br />

the remainder, however, was rejected according to the ATiOVA<br />

results,<br />

The values and plots made for the interaction of<br />

period and work/rest phases discussed above are for the<br />

combined effects of normc-:! and vibrational environments,<br />

which does not give a clear idea of the effec: of the<br />

environment upon each of these factors indiv i dL.al ly,<br />

To<br />

interpret the results obtainad in such a way a' to allow


full understanding of performance and recovery behavior<br />

105<br />

under normal and vibrational environments, performance in<br />

terms of absolute error scores was averaged over each period<br />

(average of five readings within the period), and plots of<br />

period versus average error score for each work/rest<br />

schedule under each environment, normal and vibrational,<br />

were then made, as shown in Figures 40, 41, 42, and 43.<br />

In the first work/rest schedule during which work<br />

(tracking) was performed continuously, the average error<br />

score under normal environment started high, improved<br />

slightly in the second period, leveled off in the third,<br />

then began to increase again,<br />

This behavior is anticipated<br />

in tracking tasks, in which the signal is time dependent<br />

(i,e,, repeated after a constant period of time); the<br />

subject starts at a certain levei of performance, observes<br />

the signal pattern and rate of change, learns it and performs<br />

in a more systematic way.<br />

As time passes, the task<br />

becomes boring to him and/or he becomes fatigued,<br />

The score<br />

then goes up once more,<br />

The degree of the subject's adaptation<br />

to the task, and the amount of time before he becomes<br />

fatigued depend upon the difficulty of the task« duration<br />

of exposure, arrangement of the work station, and many other<br />

factors,<br />

The decrease in error during the last of.riod of<br />

performance under normal environment (period ü) was not<br />

anticipated.<br />

It is possible that subjects expectoc the end


106<br />

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110<br />

of the run and this motivated them toward improvement in<br />

performance.<br />

Similar behavior did not occur, however,<br />

under vibratory conditions where subjects' performance<br />

decreased further during this last period,<br />

Since man<br />

himself has a time sensing ability, it is tempting here<br />

to argue that this ability could be impaired under vibratory<br />

conditions since his body senses are disrupted by engaging<br />

in vibration attenuation activity,<br />

Further research, however,<br />

is recommended before a full explanation of this behavior<br />

could be ascertained,<br />

The drop in error score at this last<br />

period of performance under normal environment is believed<br />

to have influenced the drop in error score appearlng in the<br />

same period and shown in Figure 34 (page 96),<br />

The first reading during recovery showed a continuation<br />

of the trend of the last period of performance,<br />

This<br />

was anticipated because the task performance during the<br />

first period of recovery was a continuation of the performance<br />

from the last period of work.<br />

The other two readings under recovery were taken<br />

after the work was stopped for four minutes, and they appeared<br />

to have a higher error score because of the interruption in<br />

the pattern of work which brought the subjects back to their<br />

initial levei of performance when starting a task.<br />

The average error score under a vibrational environment<br />

showed that subjects started at a certain levei of<br />

performance, and kept this for about two periods.<br />

Error


111<br />

score increased toward the end of the run, and continued<br />

to increase until vibration was stopped. Error score<br />

dropped instantaneously following cessation of vibration,<br />

then began rising again in the second and third periods<br />

of recovery, Again the rise in these two last periods<br />

is believed to be due to task interruption,<br />

During the second work/rest schedule, with subjects<br />

performing for two equally spaced fifteen-minute periods,<br />

the average error score under normal environment started<br />

high, improved after the first period probably because of<br />

subjects' adaptation to the cyclic repetition of signal,<br />

then went up again due, it is believed, to a combination<br />

of boredom and fatigue, During the second phase of work<br />

(also referred to as second trial) subjects reacted in the<br />

same way, except that their leveis of performance were<br />

even better than those during the first phase, This is<br />

believed to be due to an immediate transferal of learning<br />

from the first phase, The plotted points of the results<br />

obtained during the recovery period do not seem to support<br />

this transferal of learning explanation, It is, however,<br />

important here to mention that these points were based on<br />

one error score reading after a rest period and not an<br />

average of five readings as is plotted for the performance<br />

periods, It is therefore believed that the task interruption<br />

effect was stronger than the transfer of learning effect at<br />

these points, UJhen subjected to the vibratory environment.


112<br />

subjects' behavior in performance of the task followed the<br />

same general pattern of their performance behavior under<br />

normal environment. This is cleariy shown in Figure 41<br />

(page 107).<br />

Error scores improved significantly during<br />

the first minute of recovery immediately following vibration,<br />

then went up again in the following two periods of recovery.<br />

During the third work/rest schedule, in which subjects<br />

performed for three equally spaced ten-minute trials,<br />

the average error score under normal environment started<br />

high during the first period, and improved during the second,<br />

because of their adaptation to the task.<br />

High error scores<br />

were obtained during recovery because of the interruption of<br />

work as prevlously explained.<br />

UJhen subjected to vibratory environments, subjects'<br />

behavior in performance of the task followed closely the<br />

same trends of behavior that were noticed in performance<br />

in a normally controlled environment as shown in Figure 42<br />

(page 108).<br />

Under vibrational environment, better performance<br />

was displayed during the second and third phases of work<br />

than during the first, a condition supporting the transfer<br />

of learning explanation given earlier.<br />

Error score decreased<br />

immediately after the cessation of vibration, then increased<br />

again in the following two periods.<br />

During the fourth work/rest schddule, in which subjects<br />

performed for six equally spaced five-mj.n^:te trials,<br />

the average error score appeared to fluctuate within a narrow


113<br />

range.<br />

Performance through the last four trials under<br />

vibration displayed a slight trend toward improvement,<br />

with significant decrease in error score immediately<br />

following the cessation of vibration.<br />

Second Analysis of Variance Results<br />

The second analysis of variance was designed to<br />

test the hypotheses that work/rest schedule and period,<br />

or their interaction, affect the difference between the<br />

average error score obtained under vibration and novibration<br />

conditions.<br />

The periods under investigation<br />

include both performance and recovery periods,<br />

The<br />

results of this ANOVA are shown in Table 8,<br />

TABLE 8<br />

ANOVA FOR DIFFERENCE IN AVERAGE ERROR SCORE<br />

(VIBRATION AND RECOVERY)<br />

Source<br />

DF<br />

Sum of<br />

Squares<br />

lYlean<br />

Square<br />

F-Ratio<br />

••<br />

Blocks<br />

A, UJork/Rest<br />

5<br />

3<br />

226,61<br />

44,74<br />

37,77<br />

14,91<br />

6.85*<br />

2,70*»<br />

C, Period<br />

8<br />

98,58<br />

12.32<br />

2,23*»<br />

AC<br />

24<br />

38,72<br />

1.61<br />

0,29<br />

Error<br />

210<br />

1158.48<br />

5.52<br />

Total<br />

251<br />

1567,13<br />

* Significant at the i% levei<br />

*• Significant at the 5% levei


114<br />

The work/rest schedule had a significant effect<br />

upon average performance, under vibration at the five per<br />

cent levei,<br />

lYleans and standard deviation of the significant<br />

factor, the work/rest schedule, are given in Table 9,<br />

TABLE 9<br />

(YlEANS AND STANDARD DEVIATIONS OF 'JORK/REST SCHEDULE<br />

EFFECT ON DIFFERENCE IN AVERAGE ERROR<br />

SCORE (VIBRATION AND RECOVERY)<br />

UJork/Rest Schedule (Ylean Standard Deviation<br />

1<br />

2<br />

3<br />

4<br />

7,62<br />

7,73<br />

8,26<br />

8,57<br />

2,58<br />

2.78<br />

2.73<br />

1.65<br />

Plots of the means against the difference in average<br />

error score are shown in Figure 44.<br />

A Duncan Tilultiple<br />

Range Test indicated a significant difference between the<br />

fourth work/rest schedule (five-minute trials), and both the<br />

first schedule (thirty minutes of continuous work) and the<br />

second schedule (fifteen-minute trials).<br />

The data point to<br />

the fact that over performance and recovery peri^^ds, work/<br />

rest schedule I produced the least decrement when performed<br />

under vibration and allowed maintenance of a low average<br />

error score throughout periods of vibration and recovery.


115<br />

8,5<br />

(D<br />

P<br />

O<br />

U<br />

cn<br />

p<br />

o<br />

p<br />

P^-s<br />

Lü CO<br />

-p<br />

cn c<br />

CO ZD<br />

p<br />

CD >N<br />

> p<br />

cX CO<br />

p<br />

C -u»<br />

•H H<br />

JD<br />

CD P<br />

8,0<br />

7,5<br />

CD<br />

P<br />

CD<br />

U-<br />

(4-<br />

•H<br />

Q<br />

3<br />

UJork/Rest Schedule<br />

Fig, 44,—Plot of means of difference in average<br />

error score versus work/rest schedule (vibration and<br />

recovery),


Average difference in error score was significantly<br />

116<br />

affected by the period at the five per cent levei.<br />

Table<br />

10 gives the means and standard deviations of the effect<br />

of the significant factor:<br />

period,<br />

TABLE 10<br />

ÍYIEANS AND STANDARD DEVIATIONS OF PERIOD<br />

EFFECT ON DIFFERENCE IN AVERAGE ERROR<br />

SCORE (VIBRATION AND RECOVERY)<br />

Period (Ylean Standard Deviation<br />

1<br />

2<br />

3<br />

4<br />

5<br />

6<br />

7<br />

8<br />

9<br />

8,13<br />

8,73<br />

8,28<br />

8,62<br />

8,41<br />

8,79<br />

7,07<br />

7.09<br />

7,61<br />

1,95<br />

2,32<br />

2.60<br />

2,09<br />

1,98<br />

2,33<br />

2,92<br />

2,80<br />

2,89<br />

A Duncan (Ylultiple Range Test indicated that performance<br />

during vibrational exposure periods differed significantly<br />

from performance during recovery periods (period 7 and 8,<br />

Figure 45), No significant difference was detected during<br />

the different periods of performance under vibration,<br />

This<br />

was as expected, since cessation of vibration removes stress,


117<br />

thus allowing almost immediate recovery from its effect.<br />

Recovery is not complete, however, within the period specified<br />

for this study,<br />

This was manifested by the behavior of the ninth<br />

period (Figure 45) where difference in error score increased<br />

again•<br />

The results of the second analysis of variance<br />

indicated the validity of the hypotheses that work/rest<br />

schedule and period have a significant effect on the increase<br />

in average error score due to vibration exposure,<br />

Third Analysis of Variance Results<br />

The third analysis of variance was designed to<br />

test the hypotheses that work/rest schedule and period<br />

affect the difference between average error score obtained<br />

under vibrational environment and that obtained under normal<br />

environment,<br />

Their effect upon the percentage increase in<br />

average error score was also tested.<br />

The periods under<br />

investigation were those performed during the vibrational<br />

environment exposure only (first six periods). Table 11<br />

shows the results of the ANOVA in terms of difference in<br />

average error score.<br />

Table 11 indicates that a significant effect at the<br />

five per cent levei is attributable to the work/rest schedule.<br />

(Yleans and standard deviations of the effect of this significant<br />

factor are shown in Table 12,


118<br />

• cr><br />

00<br />

UD<br />

Ln<br />

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P<br />

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O<br />

U<br />

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OC<br />

TD<br />

O<br />

H<br />

P<br />

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CL<br />

P<br />

o<br />

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p<br />

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cn<br />

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e in ave<br />

).<br />

u >><br />

C P<br />

(D CD<br />

P ><br />

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Of diff<br />

and rec<br />

o<br />

Ln<br />

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X<br />

o<br />

,<br />

CO<br />

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ro<br />

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Fig. 45, — Pio<br />

score versus period<br />

(s^^Tun XjBj:nqjv)<br />

8JO0S JOJIJ aÕBjaAV UT aouajajjTQ


119<br />

TABLE 11<br />

ANOVA FOR DIFFERLNCE IN AVERAGE<br />

ERROR SCORE (VIBRATION)<br />

Source<br />

DF<br />

Sum of<br />

Squares<br />

íflean<br />

Square<br />

F-Ratio<br />

Blocks<br />

6<br />

84,55<br />

14.09<br />

3,03»<br />

A, UJork/Rest<br />

3<br />

47,24<br />

15.75<br />

3,38**<br />

C, Period<br />

5<br />

8,14<br />

1.63<br />

0,35<br />

AC<br />

15<br />

23,38<br />

1.56<br />

0,34<br />

Error<br />

138<br />

642,70<br />

4.66<br />

Total<br />

167<br />

806.01<br />

* S. igni<br />

i nn i<br />

ficant<br />

f 1 npjn t<br />

a t the 1^ 1 evel<br />

p t hhR Fi^í. 1 RURI<br />

TABLE 12<br />

ÍYIEANS AND STANDARD DEVIATIONS OF<br />

SCHEDULE EFFECT 01^ DIFFERENCE IN AVERAGE<br />

ERROR SCORE (VIBRATION)<br />

L'I0RK/REST<br />

UJork/Rest Schedule (Ylean Standard Deviation<br />

1<br />

2<br />

3<br />

4<br />

7.96<br />

8,04<br />

8,76<br />

9.25<br />

2,06<br />

2.55<br />

2,47<br />

1,30


120<br />

A Duncan ^ultiple Range Test indicated that work/<br />

rest schedule I and II differed significantly from work/<br />

rest schedule IV.<br />

Subjects performed better according to<br />

the first two schedules than they performed during the<br />

fourth work/rest schedule, when they were subjected to<br />

vibration. This effect is shown in Figure 46. Periods of<br />

performance during vibration exposure did not show a significant<br />

effect on difference in average error score.<br />

This was<br />

also seen prevlously in the results of the second ANOVA.<br />

This finding was in agreement with the results obtained by<br />

other experimenters in the field.<br />

Johnston (1969) found<br />

that duration of exposure does not affect performance under<br />

vibration,<br />

Results of the ANOVA in terms of percentage of<br />

increase in average error score are shown in Table 13,<br />

TABLE 13<br />

ANOVA FOR PERCENTAGE INCREASE IN ERROR<br />

SCORE (VIBRATION)<br />

Source<br />

DF<br />

Sum of<br />

Squares<br />

íil e a n<br />

Square<br />

F-Ratio<br />

Blocks<br />

A, UJork/Rest<br />

C, Period<br />

AC<br />

Error<br />

6<br />

3<br />

5<br />

15<br />

138<br />

37,80<br />

7.57<br />

1.79<br />

1.59<br />

66.69<br />

6.30<br />

2.52<br />

0.34<br />

0.11<br />

0.48<br />

13.03*<br />

5.22**<br />

0.70<br />

0.22<br />

Total<br />

167<br />

* S n ifican t<br />

** s i n n i f i rpn t at<br />

Pt<br />

115.35<br />

the 1% 1<br />

the S^^ 1<br />

evel<br />

BWBI


121<br />

CD<br />

P<br />

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p<br />

o<br />

p ^-^<br />

p CO<br />

LJ 4-><br />

•H<br />

CD C<br />

cnzD<br />

CO<br />

p >^<br />

CD P<br />

:> CO<br />

cc P<br />

-p<br />

C H<br />

•H JD<br />

P<br />

CD "^<br />

O ^—<br />

c<br />

CD<br />

P<br />

CD<br />

t»_<br />

{*-<br />

•H<br />

Q<br />

10<br />

8<br />

1 2 3<br />

UJork/Rest Schedule<br />

Fig, 45,—Plot of means for difference in average<br />

error score versus work/rest schedule (vibration).


122<br />

Table 13 demonstrates that the work/rest schedule<br />

has significant effect (at the one per cent levei) upon<br />

percentage of increase in average error during performance<br />

under vibration,<br />

Table 14 provides the means and standard<br />

deviation of the work/rest schedule effect upon percentage<br />

of increase in average error score due to vibration,<br />

TABLE 14<br />

(YlEANS AND STANDARD DEVIATIONS OF<br />

SCHEDULE EFFECT ON PERCENTAGE INCREASE<br />

IN ERROR SCORE (VIBRATION)<br />

UJORK/REST<br />

UJork/Rest Schedule lYlean Standard Deviation<br />

1<br />

2<br />

3<br />

4<br />

1,28<br />

1,32<br />

1,69<br />

1,76<br />

0,48<br />

0.68<br />

1.07<br />

0,89<br />

UJhen subjects were to perform according to the<br />

selected work/rest schedules under vibrational environment,<br />

schedules I and II resulted in significantly less percentage<br />

increase in average error score than schedules III and IV did.<br />

Figure 47 is a plot showing this result.<br />

This is believed<br />

to be due to the fact that subjects experience disturbances<br />

during vibration,<br />

UJhen instructed to begin the task, it was<br />

observed that they adjust their bodies in such a way as to<br />

attenuate the effects of the vibrational energy being


123<br />

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P<br />

O<br />

U<br />

tn<br />

p<br />

o<br />

p<br />

P^-~v<br />

UJ to<br />

-p<br />

CZ -H<br />

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C<br />

ZD<br />

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to >,<br />

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CDCO<br />

P<br />

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124<br />

transmitted to their bodies at this stage.<br />

During this<br />

adjustment process, subjects' performances are poor,<br />

After<br />

the process is complete, performance tends to improve,<br />

Since the task is cyclic, subjects adapted to it after a<br />

period of time, An example of this is shown in Figure 48,<br />

where the acceleration of the hips is attenuated gradually<br />

after the task started.<br />

The work periods not being very<br />

long, it is assumed that subjects did not reach a stage of<br />

fatigue while performing in accordance with the first two<br />

schedules, which may have nullified the improvement due to<br />

adaptation to both the task and vibration,<br />

This finding<br />

has important implications relating to the designing of<br />

phases of work and rest in tasks performed under vibrational<br />

environments.<br />

One such implication is that there may be an<br />

optimum work/rest schedule that is least affected by vibrational<br />

environment,<br />

The criteria affecting the detection of<br />

this optimum work/rest schedule are subjects' adaptation to<br />

the task, their body attenuation to vibration, and the length<br />

of work period before which they get into the stage of boredom<br />

and fatigue,<br />

Further research, however, is required in this<br />

point taking longer work period into consideration in the<br />

work/rest chedule tested,<br />

Subject effect (blocks) will not be discjsr.ed in this<br />

experiment,<br />

It may be noted that subject effect was always<br />

highly significant in ali ANOVA'5 at the one per cent levei.


Fig. 48.—Recording of • subjecfs hip acceleration<br />

before and during taak performance.<br />

125


126<br />

This was expected, of course, and even influenced selection<br />

of the model of experimental design used.<br />

This chapter has presented the results of this<br />

experiment and the interpretation of the significant<br />

findings obtained from the analysis of the data. The<br />

following chapter gives the conclusions drawn from this<br />

study and the recommendation for further research.


CHAPTER V<br />

CONCLUSIONS AND RECOíYlFílEN DAT IONS<br />

Conclusions drawn from results obtained in this<br />

investigation and presented in Chapter IV, will be discussed<br />

in this section.<br />

A comparison with the results<br />

obtained in other studies in the field will be made when<br />

appropriate, and recommendations for further research will<br />

be set out.<br />

Conclusions<br />

Environmental Effects<br />

( Environment has a highly significant effect upon<br />

human performance.<br />

A vibratory environment causes an increase<br />

in vertical tracking error.<br />

An increase in absolute error<br />

score of approximately forty-three per cent occurred under<br />

the leveis specified in this study.'<br />

This conclusion is supported in the literature by<br />

the findings of other investigators.<br />

Buckhout (1964) arrived<br />

at a similar conclusion, indicating that decrement in vertical<br />

tracking performance ranged from thirty-four to seventy-four<br />

per cent.<br />

Harris and Chiles (1964) found that at a frequency<br />

of 5 cps, and an amplitude of 0.16 inches (the leveis used<br />

in this study), a significant increase of error in the<br />

127


128<br />

vertical component of their tracking task occurred.<br />

Other<br />

investigators, also, arrived at conclusions which support<br />

those learned in the present study (Frazer, et ai., 1961;<br />

Hornick, 1961; Schmitz, 1958; and others).<br />

Period Effect<br />

i UJhen an average of performance was taken over each<br />

period (five minutes), and under both normal and vibrational<br />

environments, the difference in error score between the two<br />

did not seem to be affected by duration of exposure to<br />

vibration.^<br />

It was found that error score drops immediately<br />

in the first minute interval of the first period of recovery.<br />

It goes up again in the first minute of performance of the<br />

second and third periods of recovery, remaining, however,<br />

below that obtained under vibrational conditions,<br />

This<br />

leads to the conclusion that duration of vibration has no<br />

effect upon human performance, and that the functions of the<br />

body are performed in very much the normal way, directly<br />

after removal of stress,<br />

This improved performance is not<br />

maintained for long after recovery and the error score<br />

presently increases,<br />

This may have the sericus i^^olication<br />

that vibration at the levei specified in this study has an<br />

after exposure effect which prevents co-iplete recov.jry within<br />

as short a period of time as that employed in this study.<br />

Other investigators reached conclusions jnder the<br />

special conditions of their studies, which, u.hen analyzed.


129<br />

oxhibit decided similarities to those reached in this study,<br />

Johnston<br />

(1969), in an experiment on body orientation under<br />

vibration, concluded that the duration of exposure to vibration<br />

had no significant effect upon reaction time, travei<br />

time, accuracy, or average velocity,<br />

Faster reaction time<br />

was obtained following exposure to vibration,<br />

Simons and Hornick (1962) reported that vibration<br />

usually causes a decrement in tracking ability, and the<br />

recovery of this ability is not complete following exposure,<br />

In these studies, no differentiation was shown between<br />

performance immediately following exposure, and performance<br />

after a certain period of recovery, as was done in this<br />

experiment.<br />

Effect of UJork/Rest Schedule<br />

by Period Interaction<br />

( From the results obtained in this study it was concluded<br />

that different work/rest schedules yield different<br />

performance effects.<br />

A general performance pattern noted<br />

in the tracking task. employed is given below.<br />

This may be<br />

generalized to apply to other time-dependent and/or monotonous<br />

tasks.<br />

A subject's performance starts at a certain levei.<br />

After a warm-up period, performance improves, probably because<br />

the subject starts learning the pattern of the repeated signal,<br />

and adapts to it.<br />

After a certain time-span, performance<br />

declines again, probably because the subject becomes either


130<br />

bored, fatigued, or both.<br />

The length of this span of time<br />

depends, of course, upon the difficulty of the task, the<br />

work station, and other environmental factors.<br />

These performance characteristics appear in schedules<br />

I, II and III, in which work phases are of more than five<br />

minutes.<br />

In schedule IV, however, in which the work phase<br />

is only five minutes, the average performance appeared as one<br />

point only; therefore, these performance characteristics do<br />

not appear. This is cleariy demonstrated in Figures 40, 41,<br />

42 and 43, pages 106, 107, 108 and 109, respectively. /<br />

In order to observe the performance characteristics<br />

within each five minute period, continuous plots of performance<br />

profiles for each work/rest schedule were made (Figures<br />

51, 52, 53 and 54, Appendix D), These figures show the<br />

error score for each minute of work, rather than an average<br />

for five minutes of work, as prevlously shown in Figures 40,<br />

41, 42 and 43, pages 106, 107, 108 and 109, respectively.<br />

The profiles in these minute by minute figures Ied<br />

to a very interesting conclusion:<br />

that no matter how short<br />

the period, subject's error score following a task interruption<br />

starts high,<br />

Once he is accustomed to the signal pattern,<br />

his performance improves.<br />

This is shown to be true under ali<br />

work/rest schedules used, and explains the high error readings<br />

obtained during the second and third periods of recovery<br />

(periods 7 and 8), in which performance was measured directly<br />

after a task interruption,<br />

The continuous plot of the


eadings also showed trends similar to those prevlously<br />

131<br />

shown for the average error score over the periods.<br />

(it was concluded, also, that a subject's tracking<br />

performance follows essentially the same pattern under both<br />

normal and vibrational environments, even though the levei<br />

of performance is much better under normal environment,<br />

Under both environm!:nts a subjecfs performance starts at a<br />

certain levei, and passes through a warm-up stage, during<br />

which performance improves,<br />

It then declines in quality once<br />

more, J<br />

Another conclusion which may be drawn is that there<br />

is a process of transfer of learning,<br />

That is, if a subject<br />

were to perform a tracking task in several trials, with short<br />

periods of recovery between thfí^m, successive trials would be<br />

expected to yield an average performance as good as, or better<br />

than, that of the first trial,<br />

This is particularly true<br />

under a vibrational environment, because learning is transferred<br />

not only as pertains to the task, but possibly, also,<br />

to the subject's attenuating ability, or adjustment of his<br />

body in such a way as to weaken the effect of vibration,<br />

The process of transfer of learning was evident only<br />

during periods of controlled environment (normal and vibrational)<br />

and did not hold during periods of recovery.<br />

It is to<br />

be noted, however, that performance during the recovery period<br />

was recorded for only one minute of work (task ner f o r-.an ce).<br />

This was in comparison with an avnragc ocrforma^.-O over five


minutes of work during the controlled environment periods.<br />

As indicated prevlously, subjects always performed poorly<br />

132<br />

at the beginning of a new phase of work.<br />

It is believed,<br />

therefore, that the effect of task interruption (during<br />

recovery periods) was stronger than the effect of transfer<br />

of learning.<br />

Harris and Chiles (1964), in an experiment with<br />

vibration, and using the same leveis of frequency used in<br />

this study, reported that the performances of their subjects<br />

improved significantly through each five-trial testing period.<br />

They were tempted to postulate that the disruptive effects<br />

of vibration are temporary, and that subjects adapt to them.<br />

The results of this study support the hypothesis regarding<br />

adaptation.<br />

A temporary disruptive effect of vibration occurs<br />

only at the beginning of work trials, when subjects' bodies<br />

are not adjusted in such a way as to attenuate the vibrational<br />

effect. Performance at this point is usually poor. A detailed<br />

discussion of this point is given below.<br />

Effect of UJork/Rest Schedule upon<br />

Increase of Error Score due to Vibration<br />

UJithin the scope of this study, when work/rest schedules<br />

were put into effect under normal and vibratory environments,<br />

those with longer work phases resulted in less decrement in<br />

subject performance.<br />

This conclusion is based upon the results<br />

of two AN0VA'S.<br />

One demonstrated that the work/rest schedules<br />

used had a significant effect upon the difference in average


133<br />

error score between performance under vibration and performance<br />

in a normal controlled environment.<br />

UJork/rest schedule<br />

I, based upon thirty minutes of continuous work, affects<br />

the average increase in error score less than do other<br />

shorter work/rest schedules, especially work/rest schedule IV.<br />

Another ANOVA showed that the percentage of increase<br />

in error score under a vibrational environment, as contrasted<br />

with that under a normal environment, was also significantly<br />

affected by the work/rest schedule.<br />

Schedules having longer<br />

phases of work (schedules I and II) resulted in a lower<br />

percentage of increase in error score than did schedules<br />

having shorter work phases (schedules III and IV).<br />

í Another interesting conclusion which may be derived<br />

from the above mentioned findings is that when a subject is<br />

required to perform a task under vibration, his body utilizes<br />

its built-in vibration isolation capabilities, and adjusts<br />

itself in such a way as to attenuate the effect of vibration<br />

transmitted to it.<br />

In short, his body adapts to vibration.<br />

UJhen the task performance is stopped, the body relaxes and<br />

a disruption in body adaptation occurs.<br />

If the task is<br />

performed again after a time, the same cycle will repeat<br />

itself, and the body will attenuate vibration again.<br />

During<br />

the process of this adjustment, subject's performance is<br />

poor. I<br />

According to this study and the above hypotheses of<br />

adaptation and disruption, a recommendation might be made to


134<br />

schedule the subjects in such a way as to allow minimum<br />

disruption effects, i.e., minimum task interruption.<br />

Since, toward the end of the longer phases of work,<br />

performance tended to show a decrement, it indicated that<br />

subjects had reached a certain levei of boredom and/or<br />

fatigue.<br />

Entering this period of fatigue at a higher levei<br />

may be the limiting factor in designing the length of the<br />

work phase.<br />

A suggestion which is very tempting to make<br />

is that there might be such a thing as an optimum work/rest<br />

schedule which would result in minimum decrement when<br />

performed under a certain levei of vibration.<br />

Future<br />

research might pursue this question and try to ascertain<br />

if such an optimum work/rest schedule does, indeed, exist.<br />

Transmissibility of Vibration<br />

The frequency of vibration used in this study (5 cps)<br />

caused an amplification of acceleration transmitted from<br />

the platform to both the hip and the head.<br />

Transmissibility<br />

factors of about 1,4 between the platform and the nip, and<br />

of about 2 between the platform and the head, were noted for<br />

one experimental subject,<br />

Calculations of the accelerations<br />

transmitted are shown in Table 17, Appendix H,<br />

'his transmissibility<br />

factor varied widely from subject to subject,<br />

according to his anthropometric measurements ano ncdy structure,<br />

These leveis of acceleration transmission were<br />

observed to change when subjects moved from one posture to


135<br />

another and from a working phase to a resting phase with<br />

the body reiaxed.<br />

No attempt, however, was made to measure<br />

the amount of this change.<br />

Subjective Reaction to Vibration<br />

In this investigation, ali subjects completed ali<br />

runs without experiencing any difficulty or having to stop<br />

the vibration during any experiment.<br />

They reported a sensation<br />

of relaxation during the vibration, and immediately<br />

following it, differing sensations.<br />

Some felt dizzy; others<br />

reported an indefinable feeling best described as "floating";<br />

still others reported no effect,<br />

These feelings ended shortly<br />

after cessation of vibration and ali subjects agreed that no<br />

serious difficulty was encountered—only boredom and mild<br />

unpleasantness,<br />

The conclusion is that under the leveis of<br />

vibration used in this investigation, prolonged (one hour)<br />

exposure was withstood very well by subjects,<br />

Recommendations for Further Research<br />

This investigation gave rise to many questions deserving<br />

future research,<br />

Since vibration frequency and intensity<br />

were held constant in this study, further study extending to<br />

different leveis of vibration is recommended.<br />

As different subjects have different vibration attenuation<br />

capabilities, it would oe of interest to study the<br />

rolationship between performance and leveis of vibration


136<br />

after attenuation by the subjects.<br />

A comparison of results<br />

based upon frequency and acceleration<br />

changes is deslrable,<br />

UJork/rest schedules investigated in this research<br />

were but a few of the many which may be incorporated in a<br />

mission of one hour under continuous vibration.<br />

Future<br />

research should undertake to find the optimum<br />

work/rest<br />

schedule to be used under each levei of vibration exposure.<br />

Such an optimum may be obtained by including work/rest schedules<br />

which have longer phases of work than those used in<br />

this study, and establishing the span of work after which<br />

fatigue may occur,<br />

Research pertaining to one work/rest schedule and<br />

a comparison of this effect with that of a pretask vibration<br />

period, is also recommended,<br />

This will allow detection of<br />

the effects of vibration upon different crew members; in<br />

fact, future studies are recommended during whiuh two or<br />

more subjects are put under the same degree of vibration in<br />

a mechanical simulator, with tests being made of their efficiency,<br />

and of the mission efficiency, after changing<br />

their<br />

work/rest schedules,<br />

In this study, subjects showed conslderable<br />

improvement<br />

in their tracking ability during the last period of performance<br />

under normal environment,<br />

It was suspected that this<br />

might be due to subjects' time-sensing abilities which might<br />

have caused anticipation of the end of the task, and acted as<br />

a motivation to them, This behavior did not occur under


137<br />

vibrational conditions, however, and performance during this<br />

last period was poorer than during previous periods, It<br />

is suggested that future research investigate the effect<br />

of subjects' knowledge of the end of the task, and<br />

the<br />

effect of this upon performance, as well as the question of<br />

vibration being responsible for impairment of their timesensing<br />

abilities.<br />

Investigations concernlng recovery from vibration<br />

are still greatly needed. U/ithin the periods allowed<br />

for recovery in this study, complete recovery did not<br />

seem to occur. This could be attributable to physiological<br />

or psychological factors, The factors leading to complete<br />

recovery following vibration exposure are recommended as<br />

áreas of investigation, Since the concept of transfer of<br />

learning did not seem to hold during the recovery period,<br />

further research is required to clarify this point,<br />

Effects of vibration upon tracking behavior have<br />

been studied by many investigators. Attempts to compare<br />

their findings, however, have been very few, oractical<br />

usage of the data available is limited, It is believed that<br />

there is a great need for studies which will relate the<br />

results to a one-factor effect (i.e,, only frequency, amplitude,<br />

or acceleration),<br />

Recent development of industrial and military equipment<br />

and situations requires a great investigation of vibrational<br />

effects during long periods, It is recommonded that


138<br />

this be undertaken in future research,<br />

Long period studies,<br />

however, give rise to the question of availability of Information<br />

about safe human exposure times and tolerance limits.<br />

In spite of some excellent studies, detailed and precise<br />

Information on this subject is still lacking,<br />

Clear-cut<br />

definitions and leveis are needed, with more samples from<br />

different populations being used,<br />

In the general field of vibration studies, more<br />

interest was focused upon sinusoidal vibration,<br />

In a multitude<br />

of situations vibration is not of this kind,<br />

Random<br />

vibration is common in most vehicle operation situations,<br />

Research is recommended, therefore, in the sector of the<br />

effect of random vibration.<br />

Data upon vibrational effects in the different<br />

planes, vertical, horizontal and transverse, and combinations<br />

of these, is still needed and research should be<br />

oriented toward obtaining this Information,<br />

As was reported in this study, an effort was made<br />

to prevent ambient and vibration platform noise reaching<br />

the subjects by using cotton pieces and earphones,<br />

This<br />

arrangement is not always practlcal, and a combination of<br />

stresses might affect the subject.<br />

Studies in the sector<br />

of combined environmental stresses are needed and recommended.


139<br />

Summary<br />

This research was conducted for the purpose of studying<br />

the performance and recovery characteristics of men when<br />

subjected to relatively long periods of whole-body, vertical<br />

vibration,<br />

The effect of environment, and of a work/rest<br />

schedule, upon performance and recovery were investigated,<br />

Analysis of the performance in terms of duration of exposure<br />

to vibration was also undertaken,<br />

The significant<br />

conclusions drawn from this research are listed below:<br />

1, A vibratory environment causes significant<br />

decrement in vertical tracking ability (performance<br />

measuring task in this experiment).<br />

2, Absolute tracking error scores increased as<br />

much as 43;^ under vertical vibration,<br />

3, Duration of exposure to vibration did not<br />

affect the performance,<br />

4, Performance improved significantly immediately<br />

following the cessation of vibration,<br />

5, Complete recovery after vibration did not occur<br />

during the period allowed for recovery in this<br />

study,<br />

6, Performance of a tracking task follows a pattern<br />

in which subjects start at a certain levei of<br />

performance, experience a warm-up period during<br />

which performance improves, then display a


decline in performance,<br />

140<br />

7, Performance of the subjects improved throughout<br />

consecutive trials when they were given<br />

periods of rest between trials.<br />

8, For the work/rest schedules specified in this<br />

study, those having longer working phases<br />

showed less increase in average error scores<br />

resulting from vibration than those having<br />

shorter working phases,<br />

9, For the work/rest schedules specified in this<br />

study, those having longer working phases<br />

showed a lower percentage of increase in error<br />

score resulting from vibration,<br />

10. Acceleration was amplified when transmitted<br />

from the platform to the hip and head.<br />

11, Subjects did not have serious complaints in<br />

relation to the leveis of vibration used in<br />

this study.


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ÍYlagid, E, B,, and Coermann, R, R. Human Factors in Technology,<br />

(Bennett, et ai., eds. } New York: fílcGraw-<br />

Hill Book Company, 1963,<br />

ÍYlagid, E, B,, and Coermann, R. R. "The Reaction of the<br />

Human Body to Extreme Vibration." 1960 Proceedings,<br />

Institute of Environmental Sciences.<br />

(Ylallock, H, R, A, "Vibrations Produced by the Working of<br />

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(Ylatthews, J, "Ride Comfort for Tractor Operators," Journal<br />

of Agriculture Engineering Research, No, 1, pp, 3-<br />

31; No, 2, pp, 147-158; 1964,<br />

ÍYlcCormick, E, J, Human Factors Engineering, r.'3u York:<br />

(YlcGraw-Hill Book Company ,'1964,<br />

OlcFarland, R, A, "Human Body Size and Capabilities in the<br />

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Harvard School of Public Health, Boston, úlassachusetts,<br />

1953.<br />

rilellville, W, G, "The Vibration of Steam-Ships. " Enn ineering,<br />

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íílorgan, C, T,; Cook, J, S,; Chapanis, A.; and Lund, lYl. W,<br />

(eds,), Human Engineering Guide to Equipment<br />

Design, New York: rilcGraw-Hili Book Company, 1963.<br />

(Ylorrow, C. T. Shock and Vibration Engineering, New York:<br />

John Wiley and Sons, Inc, 1963.<br />

ÍYlozell, ÍYI, ÍYI,, and White, D, C, "Behavioral Effects of<br />

Whole Body Vibration," N ADC-ríl A-5802, í^ruject<br />

NHl 180112,4, Report No, 1, U,S. Naval Air Development<br />

Center, Johnsville, Pa., January, 1^158.<br />

niurrel, K. F. H, Human Performance in Industry. New York:<br />

Reinhold Puolishing Corporation, 1965,


150<br />

Nadei, Aaron B. "Vibration" in N, ÍYI. Burns, 'l, Chambers,<br />

and E, Hendler (eds.), iJnusual Environments and<br />

Human Behavior, TorontTi<br />

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The Free Press of Glen-<br />

Parks, D, L, "A Comparison of Sinusoidal and Random<br />

Vibration Effects on Human Performance." Document<br />

D3-3512-2, The Boeing Company, Wichita, Kansas,<br />

July, 1961.<br />

• "Defining Human Reaction to Whole Body Vibration,"<br />

Human Factors, Vol. 4, October, 1962, pp.<br />

305-314":<br />

Parks, D, L,, and Snyder, F, W, "Human Capabilities in a<br />

Vibration Environment," Technical Report, D3-3512-1,<br />

Human Factors Unit, The Boeing Company, July, 1961,<br />

Parks, D, L,, and Snyder, F, W, "Human Reaction to Low<br />

Frequency Vibration," Contract NONR 2994(00),<br />

Tech, Rep, 1, Boeing Wichita Rep. 03 3512 1,<br />

Boeing Airplane Company, Wichita, Kansas, July,<br />

1961, 65 pp,<br />

Payne, P, R, "Impact Acceleration Stress," Publication<br />

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Phillips, N, S, "A Two Degree of Freedom Analytical iTlodel<br />

to Duplicate the (Ylechanical Impedence of Seated<br />

fiílan, " Procedure of Annual Conference on Engineering<br />

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1966,<br />

Radke, A, 0. "íYlan's New Environment: Vehicle Vibration,"<br />

rnechanical Engineer, Vol, 80, July, 1958, pp, 38-41,<br />

Rathbone, T, C, "Vibration Tolerance," Power Plant Engineering<br />

, November, 1939,<br />

Rathbone, Thomas C, "Human Sensitivity to Product Vibration,"<br />

Product Engineering, Vol, 34, August 5, 1963,<br />

pp, 73-77,<br />

Reiher, H,, and (Yleister, F, J, "Die Emofindlichkeit des<br />

ÍYlenschen gegen Erschüttcrungen , " Forsch. Geb .<br />

IngWes., Vol. 2, 11, 1931, pp, 381-386,


151<br />

Reiher, H,, and ÍYleister, F, J, "Forsch, Gebiete Ingeniewrw,<br />

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It<br />

Sattinger, I, J,, et ai, "Analysis of Suspension System<br />

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Engineering Research Institute, University of<br />

ÍYlichigan, June, 1954,<br />

Schmi<br />

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Effects of Low Frequency, High Amplitude Whole-Body<br />

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Summaries of Research on the Human Performance<br />

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P-60, Aero ffledical Laboratory, Wright-Patterson<br />

Air Force Base, Ohio), 1960,<br />

Seris, H,, and Auffret, R, "rneasuremen ts of Low Frequency<br />

Vibrations in Big Helicopters and Their Transmission<br />

to the Pilot," NASA Technical Translation<br />

No, N ASA-TT-F-471, translation of "lYlesure des<br />

Vibrations de Basse Frequsnce sur Helicóptero<br />

Lourd et Transmission au Pilote," AGARD Collected<br />

Papers presented at the 22nd meeting of the AGARD<br />

Aerospace Tíledical Panei, September, 1965, pp, 245-<br />

257,<br />

Shoenberger, Richard W, "Investigation of the Effects of<br />

Vibration on Dial Reading Performance with a NASA<br />

Prototype Apollo Helmet," AíYIRL-TR-67-205, Wright-<br />

Patterson Air Force Base, Ohio, February, 1968,<br />

Sidowski, Joseph B., ed. Experimental :^lethods and Instrumentation<br />

in Psychology. New York: '>lcGraw-Hill<br />

Book Company, 1966,<br />

Simons, A, K,, and Hornick, R, J, "Effects of the Vibration<br />

Environment in Mobile Systems on Human Performance,"<br />

Ergonomics, Vol, 5, 1, January, 1962, pp, 321-327,<br />

Simons, A, K, "Tractor Ride Research." SAE Quarterly<br />

Transactions, April, 1952, pp, 357-364.


Snowden, J. C. Vibration and Shock in Damped ^^lechanical<br />

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Soliman, J. I, "A Scale for the Degrees of Vibration<br />

Perceptibility and Annoyance, Ergonomics, Vol.<br />

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"Development of a Dynamic Simulator from the<br />

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ÍYledicine and Biology, Vol. 10, 1968,<br />

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Procedure of 19th Annual Conference, 1966, 102,<br />

Suggs, C, W., and Huang, B, K, "Seat Suspension Characteristics<br />

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June, 1966, Ryksstation Voor Boerdery Boewkunde,<br />

ÍYlerelbeke (Lemberge) Gent, Belgium, 1966,<br />

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Ari1RL-TR-66-57, AD-636-317, Aerospace -ledical Research<br />

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July, 1967, pp. 6-14.<br />

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September, 1965, pp. 844-848,


154<br />

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Vertical Vibration on Respiratory Airflow and Transpulmonary<br />

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Vol. 20, September, 1965, pp, 849-c354.<br />

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Tolerance to Sinusoidal Vibration," USAF:WADC-TR-<br />

59-391, 1959,


APPENDIX<br />

A, Natural Frequencies of the Body Parts<br />

B, ÍYlonitoring Accelerometers Data and Calculations<br />

C, Example of a Subject Learning Curve<br />

D, Continuous Plots of Performance Profiles<br />

155


APPENDIX A: NATURAL FREQUENCIES OF THE BODY PARTS<br />

156<br />

TABLE 15<br />

NATURAL FREQUENCIES FOR VARIOUS PARTS OF THE BODY'<br />

Body Position or (Ylember Natural Frequency<br />

Whole body, vertical standing<br />

Whole body, prone<br />

Whole body, vertical seated<br />

Body seated on cushion<br />

Head with respect to body<br />

Lower jaw with respect to skull<br />

Shoulder and head, transverse<br />

Eyeball<br />

Hand<br />

Skull<br />

The resonance frequency of the<br />

thoracic cavity<br />

The resonance frequency of the<br />

heart<br />

The resonance frequency of the<br />

facial musculatura<br />

5 to 12 cps<br />

3 to 4 cps<br />

4 to 6 cps<br />

2 to 3 cps<br />

20 to 30 cps<br />

100 to 200 cps<br />

2 to 3 cps<br />

60 to 90 cps<br />

30 to 40 cps<br />

300 to 400 cps<br />

5 cps<br />

7 cps<br />

11 cps<br />

Compôs<br />

ited from Rathbone (1953) and Buckhout (1964)


157<br />

APPENDIX B:<br />

(YIONUORING ACCELEROÍYIE TERS DATA ANO CALCULATIONS<br />

TABLE 16<br />

SPECIFICATIONS OF THE ACCELEROíflETERS<br />

USED IN THIS STUDY<br />

Specifications<br />

Platform<br />

Hip<br />

Head<br />

Serial No.<br />

230746<br />

230726<br />

230611<br />

Reference Sensi*^i7ity<br />

at 23°<br />

50 Hz<br />

50 Hz<br />

50 Hz<br />

able Capacity of<br />

105 pF<br />

104 pF<br />

105 pF<br />

'/oltage fensitivity<br />

60.8 mV/g<br />

60,7 mV/g<br />

54.8 mV/g<br />

Change Sensitivity<br />

65,0 pC/g<br />

69,1 pC/g<br />

5G.0 pC/g<br />

Capacity (incuding<br />

cable)<br />

(Tlaximum Transverse<br />

Sensitivity at<br />

30 Hz<br />

Undamped N^jtural<br />

Frequency jndüi<br />

Tested ConditiohS<br />

'linmum ResioCancc<br />

at Room icmnerature<br />

in l;legjhms<br />

1070 pF 1138 pF<br />

1,6^<br />

1.-65^<br />

46 kHz<br />

4b kHz<br />

2ü,0ÜÜ 20,000<br />

lO^i pF<br />

3,75^<br />

46 kH7<br />

20,000


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Fig. 49.—Typical response of monitoring<br />

acclerometers.<br />

TABLE 17<br />

CALCULATION OF THE G LEVEL TR ANSíYl ITTED<br />

Specifications<br />

Platform<br />

Accelerometer<br />

Hip<br />

Placement<br />

Head<br />

Vibration<br />

frequency<br />

Recorder<br />

sensitivity<br />

Chart<br />

defIection<br />

Output<br />

voltage<br />

Accelerometer<br />

sensitivity<br />

Acceleration<br />

intensity<br />

5 cps<br />

200 mV/cm<br />

0.5 cm<br />

120 mV<br />

65.0 pC/g<br />

0.185 g<br />

5 cps<br />

200 mV/cm<br />

0.8 cm<br />

160 mV<br />

69,1 pC/g<br />

0,246 g<br />

5 cps<br />

200 mV/cm<br />

1,2 cm<br />

240 mV<br />

58,0 pC/g<br />

0,369 g<br />

Example calculation<br />

(0.6 cm) (200 mV/cm)<br />

(65.0 pC/g; (10 mV/pc)<br />

120 mV<br />

650 mV/g<br />

0,185 9


159<br />

APPENDIX C: EXAÍYIPLE OF A SUBJECT LEARNING CURVE<br />

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Fig. 50. — Example learning curve obtained "^or subject<br />

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