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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:
69<br />
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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 />
. n, ^^^' 29, —Performance on tracking tasks in relation<br />
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 />
1 I<br />
1 i<br />
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TD<br />
TD TD<br />
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cn CO cn<br />
cr cr cr<br />
TD<br />
O<br />
•H<br />
Ul<br />
(D<br />
CL<br />
CO<br />
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to<br />
u<br />
CD<br />
><br />
(D<br />
Ul<br />
O<br />
O<br />
to<br />
M<br />
O<br />
Ul<br />
Ul<br />
CD<br />
CD<br />
-P<br />
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o<br />
CO<br />
JD<br />
CD<br />
(í_<br />
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CD<br />
U<br />
C<br />
(O<br />
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Ul<br />
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u<br />
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c •<br />
CO c<br />
(D O<br />
E -H<br />
-p<br />
(*_ U<br />
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O -^-><br />
r-H C<br />
CL H<br />
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ro u.<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 />
10<br />
(D<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 />
o to<br />
u<br />
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p<br />
o<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 />
P<br />
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u<br />
cn<br />
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P<br />
cac<br />
8<br />
2 3 4 5<br />
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 />
O<br />
U<br />
cn<br />
p<br />
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o<br />
o<br />
o<br />
o<br />
o<br />
J.<br />
2 3 4 5<br />
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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108<br />
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109<br />
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to<br />
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 />
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•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 />
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o<br />
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u >><br />
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and rec<br />
o<br />
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X<br />
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,<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 />
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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 />
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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 />
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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 />
the Traffic on the Central London," Railway Board<br />
of Trade Report, 951, 1902,<br />
(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 />
Design and Operation of Vehicular Equipment,"<br />
Harvard School of Public Health, Boston, úlassachusetts,<br />
1953.<br />
rilellville, W, G, "The Vibration of Steam-Ships. " Enn ineering,<br />
Vol, 75, 33, 1903,<br />
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 />
coe, 1963, pp, 379-394.<br />
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 />
No, 977, 195-257, NAS-NRC, 1962,<br />
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 />
in ÍYledicine and Biology, Vol, 10, 1968,<br />
Poulton, E, C, "Tracking Behavior," in Acquisition of<br />
Skill, (Bilodeau, ed.). New York: Academic Press,<br />
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 />
3:177 (1932), in Shock and Vibration Handbook,<br />
C, (Yl, Harris, et ãTi (Eds, ) , New /ork: McGraij-<br />
Hill Book Company, 1961,<br />
It<br />
Sattinger, I, J,, et ai, "Analysis of Suspension System<br />
of the (Yl-47 Tank by lYleans of Simulation Techniques,"<br />
Engineering Research Institute, University of<br />
ÍYlichigan, June, 1954,<br />
Schmi<br />
Schmitz, ÍYI, A,; Simmons, A, K.; and Boettcher, C, A, "The<br />
Effects of Low Frequency, High Amplitude Whole-Body<br />
Vertical Vibration on Human Performance," In<br />
Summaries of Research on the Human Performance<br />
Effects of Vibration (W, D, Chiles and C, L, Custer,<br />
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 />
Systems. New York: john Wiley and Sons, Inc ,<br />
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152<br />
Soliman, J. I, "A Scale for the Degrees of Vibration<br />
Perceptibility and Annoyance, Ergonomics, Vol.<br />
11, 2, ÍYlarch, 1968, pp. 101-1277*^<br />
Suggs, C.^ W,; Abrams, C, F,; and Stikeleather, L, F,<br />
"Development of a Dynamic Simulator from the<br />
ÍYIechanical Impedence of Seated ÍYlan. " Procedure<br />
of the Annual Conference on Engineering in<br />
ÍYledicine and Biology, Vol. 10, 1968,<br />
Toth, R, "Engineering in (Yledicine and Biology,"<br />
Procedure of 19th Annual Conference, 1966, 102,<br />
Suggs, C, W., and Huang, B, K, "Seat Suspension Characteristics<br />
and Operator Response to Farm íYlachinery<br />
Vibration," Proceedings of XIII International<br />
Conference of Work Organization in Agriculture,<br />
June, 1966, Ryksstation Voor Boerdery Boewkunde,<br />
ÍYlerelbeke (Lemberge) Gent, Belgium, 1966,<br />
Taub, H, A, "The Effects of Vibration on Dial Reading<br />
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64-70, Aerospace (Yled, Res, Labs,, Wright-Patterson<br />
AFB, Ohio, 1964,<br />
Taub, Harvey A. "Dial-Reading Performance as a Function of<br />
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Ari1RL-TR-66-57, AD-636-317, Aerospace -ledical Research<br />
Laboratories, Aerosnace (Yledical Division, Air Force<br />
Systems Command, Wright-Patterson AFB, Ohio, July,<br />
1966,<br />
Temple, W, E,, et ai, "(Ylan's Short Time Tolerance in Sinusoidal<br />
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Toth, R. Engineering in Medicine and Biology, Proceedings<br />
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Von Gierke, H. E, "Noise and Vibration Exposure Criteria,"<br />
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1965, pp, 327-339.<br />
Von Gierke, H. E,, and Coermann, R, R, "The Biodynamics of<br />
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(Yledicine and Surgery, Vol. 32, January, 1963, pp,<br />
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under Random and Sinusoidal Vibration,"<br />
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of Simulated Buffeting on the Internai Pressure of<br />
ÍYlan," Human Factors, Vol, 4, October, 1962, pp,<br />
275-290,<br />
153<br />
Wittmann, T, J. "An Analytic ÍYlodel to Duplicate Human Dynamic<br />
Force Response to Impact." AfYlRL-TR-66-126, September,<br />
1967, Wright-Patterson Air Force Base, Ohio.<br />
Woods, A, G, "Human Response to Low Frequency Sinusoidal<br />
and Random Vibration," Aircraft Engineering, Vol. 39,<br />
July, 1967, pp. 6-14.<br />
Woodson, W, E,, and Conover, D, W, Human Engineering Guide<br />
for Equipment Designers, Berkeley: University of<br />
Califórnia Press, 1966,<br />
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"Effect of CO2 and Whole-Body Vibration on Ventilation."<br />
Journal of Applied Physiology, Vol, 20,<br />
September, 1965, pp. 844-848,
154<br />
Zechman, F. W., Jr,; Pech, D.; and Luce, E. "Effect of<br />
Vertical Vibration on Respiratory Airflow and Transpulmonary<br />
Pressure," Journal of Aopüed Physiology,<br />
Vol. 20, September, 1965, pp, 849-c354.<br />
Ziegenruecker, G, H,, and filagid, E. B, "Short Time Human<br />
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
158<br />
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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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