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Design of Spur Gears Using Profile Modification<br />

Article in Tribology Transactions · March 2015<br />

DOI: 10.1080/10402004.2015.1010762<br />

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Design of Spur Gears Using Profile Modification<br />

H. K. Sachidananda a , K. Raghunandana b & J. Gonsalvis c<br />

a School of Engineering and Information Technology, Manipal University, Dubai, 345050,<br />

United Arab Emirates<br />

b Department of Mechatronics Engineering, Manipal University, Manipal, 576104 India<br />

c St. Joseph Engineering College, Mangalore, 575001, India<br />

Accepted author version posted online: 16 Mar 2015.Published online: 26 May 2015.<br />

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To cite this article: H. K. Sachidananda, K. Raghunandana & J. Gonsalvis (2015) Design of Spur Gears Using Profile<br />

Modification, Tribology Transactions, 58:4, 736-744, DOI: 10.1080/10402004.2015.1010762<br />

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Tribology Transactions, 58: 736–744, 2015<br />

Copyright Ó Society of Tribologists and Lubrication Engineers<br />

ISSN: 1040-2004 print / 1547-397X online<br />

DOI: 10.1080/10402004.2015.1010762<br />

Design of Spur Gears Using Profile Modification<br />

H. K. SACHIDANANDA 1 , K. RAGHUNANDANA 2 , and J. GONSALVIS 3<br />

1 School of Engineering and Information Technology, Manipal University, Dubai, 345050 United Arab Emirates<br />

2 Department of Mechatronics Engineering, Manipal University, Manipal, 576104 India<br />

3 St. Joseph Engineering College, Mangalore, 575001 India<br />

Downloaded by [Manipal University], [sachidananda H K] at 21:24 26 May 2015<br />

In this work, a profile modification technique was used in<br />

design of a spur gear. In this technique, the tooth-sum is varied<br />

to obtain the desired contact ratio and low contact stress for a<br />

specified center distance. A program has been developed using<br />

C language to compute the contact stresses by varying the<br />

amount of profile shift for a tooth-sum of 100 teeth (§4%).<br />

The selected tooth-sum of 96, 100, and 104 gears was subjected<br />

to cyclic loading using a back-to-back test rig. The<br />

morphology of the damaged gear tooth surface after cyclic<br />

loading was examined by scanning electron microscopy. The<br />

morphological investigation reveals that the degree of damage<br />

observed in negative number of teeth alterations is less<br />

compared to standard and positive alteration tooth-sum due to<br />

lower contact stress.<br />

KEY WORDS<br />

Gears, Spur Gears, Scoring, Scuffing, Fatigue, Rolling-Contact<br />

Fatigue<br />

INTRODUCTION<br />

The contact stress is an important factor to maintain durability<br />

of the contact surface of external meshing gears (Nabih, et al.<br />

(1)). Hence, stress analysis in the contact area and assessing the<br />

most critical conditions are of particular interest to the appropriate<br />

design of the transmission gears (Ruben, et al. (2)).<br />

To determine the critical points (which have higher contact<br />

stress) and critical conditions in a mating gear requires complex<br />

calculations. In this context, many researchers made attempts<br />

and found solutions. Stachowiak and Batchelor (3) estimated<br />

contact stresses on nonconformal surfaces (spur gears) by analytical<br />

equations based on the elasticity theory developed by Hertz.<br />

Miryam, et al. (4) also used the Hertz equation in combination<br />

with a model of load distribution along the line of contact to<br />

compute contact stress in spur and helical gears. They also<br />

reported that the load distribution is not uniform (due to the<br />

change in rigidity of the pair of teeth) along the path of contact<br />

and has a decisive influence on the location and magnitude of<br />

the contact stress. Valentin (5) reported that the continuous<br />

Manuscript received November 3, 2014<br />

Manuscript accepted January 17, 2015<br />

Review led by Robert Errichello<br />

Color versions of one or more of the figures in the article can be found<br />

online at www.tandfonline.com/utrb.<br />

736<br />

interaction between the profile form and contact parameters<br />

should be considered in designing models for gear teeth (Hayrettin<br />

(6)). Fatih and Stephen (7) showed that the wear at the beginning<br />

and end of the tooth mesh due to instantaneous contact<br />

loads and Hertz pressures is also a parameter that affects tooth<br />

performance.<br />

Further, in some of the literatures (Ali (8); Sfakiotakis, et al.<br />

(9)), it is found that the stress distribution in gear teeth is an<br />

elliptical pattern and the maximum stresses are in the middle<br />

and are computed by Eq. [1]:<br />

vffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffi<br />

<br />

u<br />

Q 1 R 1<br />

C 1 R 2<br />

s max D t h<br />

i: [1]<br />

bp 1 ¡ #2 1<br />

E 1<br />

C 1 ¡ #2 2<br />

E 2<br />

An improvement over the Hertzian theory was provided by<br />

Johnson (10), according to which the contact stress is influenced<br />

by the adhesiveness of the surfaces in contact and the correlation<br />

between the contact area, the elastic material properties, and<br />

interfacial interaction strength.<br />

As per BS ISO 6336-2 (11) standard for gears with a contact<br />

ratio range of 1 to 2, the nominal contact stress is to be determined<br />

at the pitch point. The contact stress at the inner limit<br />

(single-pair tooth contact) on the pinion or wheel is to be determined<br />

using the single-pair tooth contact factors Z B (pinion) or/<br />

and Z D (wheel; Shuting (12)).<br />

In meshing gears, defects like pitting, scoring, scuffing, and<br />

wear due to fatigue effects are common defects on the tooth<br />

surface. These defects are due to maximum Hertz surface<br />

pressure (Anders and Soren (13)) and fluctuating load. When<br />

gears operate at maximum load capacity, a very high contact<br />

pressure occurs at the mesh interference. This leads to partial<br />

breakdown of the lubricant and causes mild wear, scuffing,<br />

scoring, spalling, and pitting (Amarnath and Sujatha (14)).<br />

The sudden tooth load changes at lowest point of singletooth<br />

contact (LPSTC), and the highest point of single-tooth<br />

contact (HPSTC) causes fluctuations in contact stresses (Li<br />

and Kahraman (15)). The fluctuation in contact stress also<br />

causes fatigue, which leads to pitting at the contact surfaces<br />

and generally involves combined rolling and relative sliding<br />

actions.<br />

It is seen that most of the literature pertains to contact<br />

stress analysis using standard gearing. The literature on stress<br />

analysis of altered tooth-sum gearing is limited. As the


Design of Spur Gears Using Profile Modification 737<br />

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NOMENCLATURE<br />

a D Center distance (mm)<br />

b D Face width (mm)<br />

E 1 D Young’s modulus (pinion) (MPa)<br />

E 2 D Young’s modulus (gear) (MPa)<br />

F n D Normal force (N)<br />

GSL D Top land width (gear) (mm)<br />

m D Module (mm)<br />

P bn D Base pitch (mm)<br />

PSL D Top land width (pinion) (mm)<br />

Q D Load (N)<br />

R 1 D Radius of curvature (pinion) (mm)<br />

R 2 D Radius of curvature (gear) (mm)<br />

R max1 D Maximum radius permitted (pinion) (mm)<br />

R max2 D Maximum radius permitted (gear) (mm)<br />

r D Radius (mm)<br />

profile shift varies, the value of contact stress also changes,<br />

which has not been explored in detail for altered tooth-sum<br />

gearing. Authors in this context made attempts to investigate<br />

contact stress analyses of altered tooth-sum gearing for 40<br />

tooth-sums to 240 tooth-sums in steps of 20 tooth-sums<br />

(Sachidananda, et al. (25, 26)). In that research finding, they<br />

reported that it is possible to predict the contact stress and<br />

tailor the design of gears for high contact ratio (lower contact<br />

stress) by altering the tooth-sum gearing. Based on this<br />

research output, it is also found that further investigation of<br />

a particular tooth-sum (100 § 4%) gearing that is commonly<br />

used in private and public transportation vehicles is needed.<br />

In addition to stress analysis, the location of maximum contact<br />

stress points and morphological investigation at critical<br />

points needs to be determined. In view of the above literature<br />

gap, the authors extended earlier work and reported in<br />

this article an investigation of the contact stress in commonly<br />

used altered tooth-sum gearing (100) and its locations by<br />

varying the amount of profile shift. In addition, morphological<br />

investigation of contact surfaces of the tooth were carried<br />

out to determine the types of damage.<br />

METHODOLOGY<br />

Parameters Considered for Computation<br />

The geometrical parameters considered for computing contact<br />

stresses are module of 2 mm, face width of 20 mm, and pressure<br />

angles of 20 and 25 . The material for the gear considered was<br />

steel (C40) and the Young’s modulus of the material was taken<br />

as 200 GPa. The applied tangential tooth load of 10 N per unit<br />

millimeter of face width was taken to compute the contact stress.<br />

Estimation of Contact Stress<br />

The following methodology has been used to compute the<br />

contact stress for altered tooth-sum for various values of profile<br />

shift.<br />

r 11 D Pitch circle radius (pinion) (mm)<br />

r 12 D Pitch circle radius (gear) (mm)<br />

r a1 D Addendum circle radius (pinion) (mm)<br />

r a2 D Addendum circle radius (gear) (mm)<br />

r b1 D Base circle radius (pinion) (mm)<br />

r b2 D Base circle radius (gear) (mm)<br />

X D Profile shift coefficient (mm)<br />

X 1 D Profile shift coefficient (pinion) (mm)<br />

X 2 D Profile shift coefficient (gear) (mm)<br />

e D Contact ratio<br />

s max D Contact stress (MPa)<br />

y 1 D Poisson’s ratio (pinion)<br />

y 2 D Poisson’s ratio (gear)<br />

f D Standard pressure angle ( )<br />

f W D Working pressure angle ( )<br />

The maximum contact stress induced was calculated based on<br />

Eq. [2] (Fernandes and Mcduling; Moldovan, et al. (19)):<br />

sffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffi<br />

0:35Q 1 R1<br />

s max D<br />

C <br />

1<br />

R2<br />

b 1<br />

E1 C <br />

1 : [2]<br />

E2<br />

The profile shift (X) for each tooth-sum altered has been calculated<br />

by Eq. [3] (Gitin (20)):<br />

½inv f<br />

X D Z w ¡ inv fŠ<br />

e : [3]<br />

2 tan f<br />

Figure 1a shows the different points along the path of contact<br />

of meshing gears, which are identified as A, B, C, D, and E.<br />

Figures 1b and 1c indicate the load distribution along the path of<br />

contact as the contact ratio ranges from 1.2 to 2 and greater<br />

than 2, respectively.<br />

For any external gear pair, the pitch point C keeps a constant<br />

position on the centerline of the gear, whereas points A, E and<br />

points B, D, the single-pair gear meshing segments, change their<br />

position along the theoretical gear segment T 1 T 2 . The influence<br />

over the position of points A, E and points B, D is given by the<br />

profile shift distribution between the gear pair and gear ratio in<br />

order to maintain the normal addendum clearance between<br />

teeth. In this analysis, the influence of profile shift on these<br />

points AE and points BD have been considered.<br />

The radius of curvature and maximum contact stress at different<br />

points along the length of the path of the contact is computed<br />

from the following set of equations (refer to Fig. 1). The steps<br />

followed to compute the radius of curvature are as follows<br />

(Gitin (20)):<br />

T 1 T 2 D a sin ; w [4]<br />

qffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffi<br />

T 1 A D T 1 T 2 ¡ ra2 2 ¡ r2 b2<br />

[5]<br />

T 2 A D T 1 T 2 ¡ T 1 A [6]<br />

qffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffi<br />

T 1 B D ra1 2 ¡ r2 b1<br />

¡ P bn ; [7]


738 H. K. SACHIDANANDA ET AL.<br />

Downloaded by [Manipal University], [sachidananda H K] at 21:24 26 May 2015<br />

Fig. 1—Path of contact from beginning to end described as A, B, C, D, and E. A, beginning of contact; B 1 , end of two-pair mesh; B 2 , beginning of singlepair<br />

mesh; C, pitch point; D 2 , end of single-pair mesh; D 1 , beginning of two-pair mesh; E, end of contact.<br />

where P bn D p m cos f.<br />

T 2 B D T 1 T 2 ¡ T 1 B [8]<br />

T 1 C D ða sin f W Þ=2 [9]<br />

T 2 C D T 1 T 2 ¡ T 1 C [10]<br />

qffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffi<br />

T 1 D D T 1 T 2 ¡ ra2 2 ¡ r2 b2<br />

C P bn [11]<br />

T 2 D D T 1 T 2 ¡ T 1 D [12]<br />

qffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffi<br />

T 1 E D ra1 2 ¡ r2 b1<br />

[13]<br />

T 2 E D T 1 T 2 ¡ T 1 E: [14]<br />

The steps followed to compute the contact ratio ( 2 ) are as follow<br />

(Gitin (20)):<br />

2D T 1E ¡ T 1 A<br />

P bn<br />

: [15]<br />

The maximum radius permitted without any interference for the<br />

pinion and gear is given by (Gitin (20))<br />

qffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffi<br />

R max1 D R 2 b1 C ð a sin f wÞ 2<br />

[16]<br />

(Gitin (90)):<br />

<br />

f w D cos ¡ 1 Z e cosf<br />

; [18]<br />

Z<br />

where Z e is the altered tooth-sum and Z is the standard toothsum.<br />

The addendum radius of the pinion and gear was calculated<br />

using the following set of equations (Gitin (20)):<br />

R a1 D ða C m ¡ x 2 mÞ¡ r 12 [19]<br />

R a2 D ða C m ¡ x 1 mÞ¡ r 11 : [20]<br />

where r 11 and r 12 are the pitch circle radii of the pinion and gear.<br />

The restricting conditions are maximum radius permitted as follows<br />

(Li and Kahraman (15)):<br />

R max1 R a1 and R max2 R a2 : [21]<br />

In addition to the above condition, the top land width of the<br />

pinion and gear should satisfy the following condition (Gitin<br />

(20)):<br />

PSL 0:25 m and GSL 0:25 m: [22]<br />

The individual radius of curvature at different points along the<br />

length of path of contact is calculated using Eq. [23] (Fernandes<br />

and Mcduling (19)):<br />

qffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffi<br />

R max2 D R 2 b2 C ð a sin f wÞ ; [17]<br />

ðRTR<br />

Þ X<br />

D T 1XðT 1 T 2 ¡ T 1 XÞ<br />

; [23]<br />

T 1 T 2<br />

where f w is the change in pressure angle and is called the working<br />

pressure angle and calculated using the following equation<br />

where X stands for different points along the length of the path<br />

of contact (A, B 1 ,B 2 ,C,D 1 ,D 2 , and E).


Design of Spur Gears Using Profile Modification 739<br />

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The normal force along the different points along the length of<br />

path of contact was calculated using Eq. [24]:<br />

F t<br />

FNX D ; [24]<br />

cos tan ¡ 1<br />

where F t is the tangential force (N).<br />

The individual load along the different points on the length of<br />

the path of contact was calculated using Eq. [25]:<br />

T 1 X<br />

R b1<br />

QX D FNX<br />

b ; [25]<br />

where b is the face width (mm).<br />

The maximum contact stress along different points on the<br />

length of the path of contact was calculated using Eq. [26]:<br />

where<br />

sffiffiffiffiffiffiffiffiffiffiffiffiffiffiffi<br />

QX<br />

.s max / X D con ; [26]<br />

ðRTR<br />

rffiffiffiffiffiffiffiffiffiffiffiffi<br />

0:35E<br />

con D<br />

2<br />

Þ X<br />

[27]<br />

if the pinion and gear are of the same material.<br />

A computer program was developed based on the above<br />

methodology using C language to compute the contact stresses.<br />

Experimental Investigation<br />

Figure 2 shows the digital photograph of back-to-back cyclic<br />

loading experimental test rig. It is one of the standard test rigs<br />

used to test gears for finite life fatigue (Nabih, et al. (1)). In the<br />

present research work, a selected tooth-sum of 96, 100, and 104<br />

gears was tested for a total of 10 6 cycles.<br />

Fig. 2—FZG testing machine used for experimentation. 1, Gear train<br />

under test (heat treated); 2, shaft; 3, torque meter; 4, vernier<br />

coupling; 5, support plate; 6, transmission gear (untreated).<br />

Subsurface cracks, multiple cracks on the surface, scuffing,<br />

and pitting are the surface defects that are commonly developed<br />

during fatigue loading of gear teeth. In this work, in order to<br />

obtain a clear picture of surface damage, a morphological study<br />

of the tested gear tooth was conducted using scanning electron<br />

microscopy (SEM; JEOL-JSM-6380LA, Japan). The samples<br />

were prepared by wire electrodischarge machining at appropriate<br />

points on the gear tooth and the sample surface was coated<br />

with gold using a sputtering unit. SEM microphotographs were<br />

taken at appropriate voltage.<br />

RESULTS AND DISCUSSION<br />

Contact Stress<br />

The s max point shifts along the path of contact and it depends<br />

on profile shift and position of pitch point C. It is shown in<br />

Fig. 1a that T 1 C > T 1 B; hence, the ratio T1C<br />

T >1 and s 1B max for the<br />

pinion appears at point B. Otherwise, if T 1 C T 1 B, the ratio T1C<br />

T 1B<br />

1 and s max for the pinion appears at point C. Similarly, if T 2 C<br />

> T 2 D, and if T 2 C T 2 D, the s max for the gear appears at points<br />

D and C, respectively (Moldovan, et al. (24)).<br />

The length of T 1 T 2 for 100 tooth-sum gears altered by §4%<br />

for 20 and 25 pressure angles was computed using Eq. [4] and<br />

tabulated as shown in Table 1.<br />

Based on the these tabulated values, the ratio of contact<br />

lengths versus profile shift for 20 and 25 pressure angles was<br />

computed using the developed C program and the plots were<br />

drawn as shown in Fig. 3. The ratio of T1C T2C<br />

T 1B<br />

and<br />

T at s 2D max point<br />

for 20 and 25 pressure angles was identified by the output and<br />

tabulated as shown in Table 2. The computed values of contact<br />

ratio, addendum, dedendum, and whole depth using C program<br />

were compared with the appendix F and appendix D in Gitin<br />

(20) and it was found that the values are in line.<br />

From the ratio of contact lengths versus profile shift plots<br />

(refer to Fig. 3), the following analysis was made. The ratio T1C<br />

T 1B<br />

decreases and the ratio T2C<br />

T 2D<br />

increases with an increase in profile<br />

shift on the pinion. The range of profile shift (X 1 ) for a 20 pressure<br />

angle varies between ¡0.6 to 1 and ¡1.6 to 0.6 for negative<br />

and positive alteration tooth-sum, respectively. Similarly, the<br />

range of profile shift for 25 pressure angle varies between ¡0.6<br />

to 1.8 and ¡1.8 to 0.7 for negative alteration and positive alteration<br />

tooth-sum, respectively. From Table 2, it is seen that for a<br />

tooth-sum of 96 teeth the ratio T1C<br />

T 1B<br />

is 1.014 for the profile shift<br />

X 1 D 1.6 and the ratio T1C<br />

T is 0.996 for profile shift X 1B 1 D 1.7 for a<br />

20 pressure angle. This indicates that s max shifts from point B to<br />

point C. Similarly, for the same tooth-sum the ratio of T2C<br />

T 2D<br />

is 0.984<br />

for the profile shift X 1 D 0.3 and 1.001 for the profile shift X 1 D<br />

0.4, where the s max shifts from point C to point D. These are the<br />

critical points where s max shifts from the inner contact point (B)<br />

of a single-pair mesh to the pitch point (C) and vice versa.<br />

In general, from Table 2, for negative alteration (96, 97, 98,<br />

and 99) tooth-sum and for standard tooth-sum (100), it is seen<br />

that the ratio of T1C T2C<br />

T 1B<br />

and<br />

T 2D<br />

changes from point B to point C and<br />

from point C to point D for positive values of profile shift. Similarly,<br />

for positive alteration (101, 102, 103, and 104) in tooth-sum


740 H. K. SACHIDANANDA ET AL.<br />

TABLE 1—LENGTH OF PATH OF CONTACT (MM) FOR TOOTH-SUM OF 100 ALTERED BY §4TEETH<br />

Altered tooth-sum 96 97 98 99 100 101 102 103 104<br />

Length of T 1 T 2 (’ D 20 ) 43.15 41.13 38.98 36.68 34.2 31.5 28.51 25.14 21.2<br />

Length of T 1 T 2 (’ D 25 ) 49.22 47.66 45.95 44.15 42.26 40.26 38.14 35.86 33.41<br />

Downloaded by [Manipal University], [sachidananda H K] at 21:24 26 May 2015<br />

the ratio of T1C<br />

T 1B<br />

T2C<br />

and<br />

T 2D<br />

changes from point B to point C and point<br />

C to point D for negative values of profile shift.<br />

The magnitude and point of s max for altered tooth-sum gearing<br />

has been computed by C program and tabulated in Table 3.<br />

The following salient features were observed from Table 3. It is<br />

seen from the results at a profile shift of 1.6 the s max is in a single-pair<br />

mesh (point B). For f D 20 and X 1 D 1.6 it is seen that<br />

value of s max for a tooth-sum of 96 at point C is 189.48 MPa. In<br />

this case, the length of T 1 C is greater than T 1 B (21.57 mm ><br />

21.27 mm) and T 1 C is less than T 1 E (27.17 mm). Hence, the<br />

s max is at pitch point C, which lies in a single-pair mesh between<br />

point B and point D. For the same tooth-sum, the value of s max<br />

for the profile shift X 1 D 1.7 at point C is 133.98 MPa, which is<br />

less compared to previous value of profile shift and is due to<br />

smaller length of T 1 C (21.57 mm), which is less than T 1 B<br />

(21.65 mm). Therefore, the magnitude of s max is reduced as the<br />

pitch point C lies in between point A and point B (two-pair<br />

mesh). In addition, for f D 25 and X 1 D 1.6, a similar trend was<br />

observed.<br />

It is observed that the magnitude of s max at points B and C is<br />

lower at a 25 pressure angle compared to a 20 pressure angle<br />

for profile shifts of 1.6 and 1.7. The length of the path of contact<br />

T 1 T 2 is 49.22 mm in the case of a 25 pressure angle is higher<br />

compared to the length of the path of contact at a 20 pressure<br />

angle (43.15 mm). This leads to an increased radius of curvature<br />

and results in reduced contact stress.<br />

In the case of f D 20 , X 1 D 0.1, and tooth-sum of 100, the s max<br />

at pitch point C is 208.53 MPa, and the length of T 1 C is greater<br />

than T 1 B (17.10 mm >16.84 mm) and less than T 1 D (18.29 mm).<br />

The pitch point C lies in between point B and point D; hence, C<br />

lies in a single-pair mesh. In this case, the contact ratio is 1.75.<br />

Similarly, for f D 25 for the same tooth-sum, the s max at point<br />

Fig. 3—Plots of ratio of contact lengths versus profile shift: (a) (T 1 C)/(T 1 B) versus X 1 and (b) (T 2 C)/(T 2 D) versus X 1 for a 20 pressure angle; (c) (T 1 C)/(T 1 B)<br />

versus X 1 and (d) (T 2 C)/(T 2 D) versus X 1 for a 25 pressure angle.


Design of Spur Gears Using Profile Modification 741<br />

TABLE 2—RATIO T1C<br />

T 1B AND T 2C<br />

T 2 D AT s MAX POINT FOR 20 AND 25 PRESSURE ANGLES<br />

For f D 20 <br />

For f D 25 <br />

Altered tooth-sum X 1 T 1 C/T 1 B X 1 T 2 C/T 2 D X 1 T 1 C/T 1 B X 1 T 2 C/T 2 D<br />

Downloaded by [Manipal University], [sachidananda H K] at 21:24 26 May 2015<br />

96 1.6 1.014 0.3 0.984 1.6 1.012 0.4 0.988<br />

1.7 0.996 0.4 1.001 1.7 0.998 0.5 1.002<br />

97 1.2 1.019 0.2 0.991 1.3 1.011 0.3 0.994<br />

1.3 0.999 0.3 1.01 1.4 0.996 0.4 1.01<br />

98 0.8 1.013 0.1 0.998 0.9 1.011 0 0.998<br />

0.9 0.992 0.2 1.02 1 0.995 0.1 1.004<br />

99 0.5 1.006 0 0.984 0.7 1 ¡0.1 0.995<br />

0.6 0.985 0 1.008 0.8 0.983 0 1.012<br />

100 0.1 1.015 ¡0.2 0.989 0.3 1.005 ¡0.4 0.987<br />

0.2 0.989 ¡0.1 1.015 0.4 0.987 ¡0.3 1.005<br />

101 ¡0.2 1.027 ¡0.3 0.998 0 1.018 ¡0.5 0.994<br />

¡0.1 0.996 ¡0.2 1.03 0.1 0.998 ¡0.4 1.015<br />

102 ¡0.4 1.028 ¡0.5 0.998 ¡0.3 1.015 ¡0.8 0.982<br />

¡0.3 0.999 ¡0.4 1.036 ¡0.2 0.993 ¡0.7 1.004<br />

103 ¡0.5 1.031 ¡0.9 0.966 ¡0.5 1.015 ¡0.9 0.999<br />

¡0.4 0.985 ¡0.8 1.009 ¡0.4 0.991 ¡0.8 1.015<br />

104 ¡0.4 1.019 ¡1.4 0.993 ¡0.8 1.025 ¡1.1 0.997<br />

¡0.3 0.961 ¡1.3 1.005 ¡0.7 0.996 ¡1 1.025<br />

C is 191.02 MPa for profile shift X 1 D 0.3 and lies in between<br />

point B and point D. However, the magnitude of s max was lower<br />

in the 25 pressure angle compared to the 20 pressure angle.<br />

For f D 20 , X 1 D¡0.4, and tooth-sum of 104 teeth, it has<br />

been noted that the s max at point C is 150.21 MPa. In this case,<br />

the length of T 1 C is smaller compared to T 1 B (10.60 mm <<br />

13.32 mm). Point C is in between point A and point B and falls<br />

in a two-pair mesh. In this case, the contact stress is lower<br />

because the contact ratio is 2.01 (two pairs of teeth are lifting the<br />

load). However, for the same tooth-sum the s max is high for a<br />

TABLE 3—MAGNITUDE AND POINT OF s MAX FOR ALTERED TOOTH-SUM GEARING<br />

Altered<br />

s max at<br />

Tooth-sum X 1 B 1 (Mpa)<br />

For f D 20 <br />

s max at<br />

B 2 (Mpa)<br />

25 pressure angle compared to a 20 pressure angle. This is due<br />

to fact that the pitch point C lies in between point B and point D<br />

and falls in a single-pair mesh with a contact ratio of 1.68.<br />

From Table 3 it is observed that the value of contact stress at<br />

point B 1 and point B 2 increases up to a tooth-sum of 102 for a<br />

20 pressure angle as the tooth-sum increases. Further, the<br />

observed increased tooth-sum (103 and 104) decreased the magnitude<br />

of the contact stress. This is due to the reduction in length<br />

of T 1 C.Fora25 pressure angle it is seen that the value of contact<br />

stress at point B 1 and point B 2 continuously increases from<br />

s max at<br />

s max at<br />

C (Mpa) X 1 B 1 (Mpa)<br />

For f D 25 <br />

s max at<br />

B 2 (Mpa)<br />

s max<br />

at C (Mpa)<br />

96 1.6 133.81 189.24 189.48 1.6 127.46 180.25 180.52 B<br />

1.7 133.81 189.24 133.98 1.7 127.67 180.55 127.64 C<br />

97 1.2 136.44 192.65 193.25 1.3 129.23 182.62 182.83 B<br />

1.3 136.44 192.65 136.65 1.4 129.35 182.93 129.3 C<br />

98 0.8 139.39 197.13 197.32 0.9 130.74 184.84 185.06 B<br />

0.9 139.39 197.13 139.52 1 130.91 185.14 130.85 C<br />

99 0.5 143.14 202.43 202.52 0.7 132.94 188.01 188.01 B<br />

0.6 143.14 202.43 143.2 0.8 133.19 188.36 132.94 C<br />

100 0.1 147.34 208.37 208.53 0.3 135 190.93 191.02 B<br />

0.2 147.34 208.37 147.45 0.4 135.24 191.26 135.07 C<br />

101 ¡0.2 152.81 216.1 216.31 0 137.69 194.63 194.89 B<br />

¡0.1 152.81 216.1 152.96 0.1 137.83 194.12 137.81 C<br />

102 ¡0.4 159.78 225.96 159.9 ¡0.3 140.65 198.91 199.11 B<br />

¡0.3 159.78 225.96 226.36 ¡0.2 140.86 199.21 140.79 C<br />

103 ¡0.5 138.33 169.42 138.4 ¡0.5 144.44 204.27 204.46 B<br />

¡0.4 138.33 169.42 169.65 ¡0.4 144.66 204.58 144.57 C<br />

104 ¡0.4 149.91 183.61 150.21 ¡0.8 148.81 210.46 210.68 B<br />

¡0.3 149.91 183.61 183.97 ¡0.7 149 210.72 148.97 C<br />

Point<br />

of s max


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742 H. K. SACHIDANANDA ET AL.<br />

Fig. 4—Gear tooth surface morphology: (a) 96 tooth-sum (point B), (b) 96 tooth-sum (point D), (c) 100 tooth-sum (point B), (d) 100 tooth-sum (point D),<br />

(e) 104 tooth-sum (point B), and (f) 104 tooth-sum (point D).<br />

96 teeth to 104 teeth due to a continuous decrease in the radius<br />

of curvature from negative alteration to positive alteration in<br />

tooth-sum.<br />

The s max for negative alteration in tooth-sum is lower<br />

compared to standard tooth-sum for both 20 and 25 pressure<br />

angles. Similarly, for a tooth-sum of 103 the contact<br />

stress induced is lower compared to a standard tooth-sum for<br />

f D 20 even though the length of T 1 T 2 is smaller compared<br />

to a standard tooth-sum. This is due to a negative profile<br />

shift for both pinion and gear compared to a positive shift in<br />

standard gearing.<br />

The s max for negative alteration in tooth-sum is lower compared<br />

to a standard tooth-sum. This is due to the longer length of<br />

T 1 T 2 . However, the magnitudes of contact stresses were higher<br />

for positive alteration in tooth-sum compared to a standard<br />

tooth-sum. From Table 3 it is seen that negative alteration in<br />

tooth-sum performed better compared to a standard tooth-sum<br />

from a contact stress point of view and the stresses are much


Design of Spur Gears Using Profile Modification 743<br />

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lower in a 25 pressure angle compared to a 20 pressure angle.<br />

This analysis holds for changing of s max from point C to point D<br />

similar to point B and point C. The behavior of altered toothsum<br />

gearing performs in the same way as discussed above for<br />

changing of points from point C to point D.<br />

Morphological Investigation<br />

Generally, to ensure long-term transmission reliability in<br />

automotive vehicles the gear designer must consider requirements<br />

such as high static strength, bending fatigue, and rolling<br />

contact fatigue (William and Richard (30)). In particular, rolling<br />

contact fatigue cracks are one of the most important problems<br />

for gears (Aslantas and Tasgetiren (16); Vera and Ivana (29)).<br />

Under rolling contact, various surface damage (pitting, spalling,<br />

and cracking) occurs and cracks develop in the gear tooth surface,<br />

thus leading to loss of serviceability of the gear (Anders<br />

and Soren (13); Singh, et al. (28)). Both macro- and microcracks<br />

lead to surface damage, and subsurface cracks generate heavy<br />

surface damage like pitting. In most material failures, tensile<br />

stresses appear to be the common mode and the material surface<br />

is stretched or pulled apart, thus leading to microscopic surface<br />

cracking and macroscopic-scale pitting or spalling (Dimitrov,<br />

et al. (17); Michele and Giuseppe (23)).<br />

In a meshing gear pair LPSTC to the HPSTC only one pair of<br />

gear tooth in contact and the normal force is higher for this<br />

region. Below the LPSTC and above the HPSTC there is more<br />

than one pair in contact (Marco, et al. (22)). Hence, in the present<br />

investigation point B (LPSTC) and point D (HPSTC) on the<br />

pinion are the critical points of contact that are considered in<br />

gears for rolling type of failure. In this context, 96, 100, and 104<br />

tooth-sum gears were selected for experimentation and are subjected<br />

to fatigue loading. The surfaces at point B (LPSTC) and<br />

point D (HPSTC) on the tested pinion tooth surface were<br />

selected and specimens were prepared for morphological investigations.<br />

SEM micrographs of these surfaces are shown in Fig. 3.<br />

In the experimental results, it is observed that pitting failures<br />

occur roughly between the initial point of a single-tooth contact<br />

(point B) and pitch point C and from pitch point C to the final<br />

point of the single-tooth contact (point D) because these are the<br />

points of highest load when the contact ratio is greater than 1.2<br />

and less than 2.<br />

Figures 3a and 3b show SEM micrographs of the pinion tooth<br />

surface at points B and D for a tooth-sum of 96. The sum of the<br />

profile shift coefficient is 2.27 mm and in this case both gear and<br />

pinion wer generated with equal amounts of profile shift and the<br />

maximum contact stress at point B 1 is 189.48 MPa. This is the initial<br />

point of the single-tooth contact. Microcracks are observed<br />

at point B (Fig. 3a, higher magnification) and multiple macrocracks<br />

are observed at point D (Fig. 3a, higher magnification). It<br />

is found that the crack intensity and number of cracks are greater<br />

at point D compared to point B. This is due to s max at D. From<br />

these micrographs it can be seen that the surface deterioration at<br />

the region of point D is greater compared to that at point B. In<br />

driving and driven members the sliding direction and rolling are<br />

opposite each other (as observed in all SEM micrographs) and<br />

cracks grow opposite to the direction of sliding.<br />

Figures 3c and 3d show SEM micrographs of 100 tooth-sum<br />

pinion teeth surfaces at points B and D. From Figs. 3c and 3d it<br />

is seen that the surface damage is more severe at point B (Fig. 3c,<br />

lower magnification) compared to point D (Fig. 3d, higher magnification).<br />

However, plastic deformation is observed on the surface<br />

in both points of contacts. This is due to the kinematic<br />

characteristics of the gear teeth contact and teeth lubricating<br />

conditions (Joze and Gorazd (21)). It can be stated that the more<br />

aggressive the contact conditions and a thin lubricating specific<br />

film thickness lead to plastic deformation and a feather edge<br />

forms due to plastic flow of material (Fig. 3c; Errichelo (18)).<br />

Scuffing (scoring) is a form of gear tooth surface damage that<br />

occurs due to the absence or breakdown of a lubricant film<br />

between the contacting surfaces of the mating gears (Vera and<br />

Ivana (29); Sheng and Ahmet (27)). Figures 3e and 3f show the<br />

micrographs of 104 tooth-sum pinion teeth surfaces at points B<br />

and D. It can be seen from Table 3 that the contact stress is at<br />

point B and remains the same at point D because of the two-pair<br />

mesh. Though the maximum contact stress value in this case is<br />

lower than in the above two cases, the contact ratio in this case is<br />

2.07, which is higher. This leads to a shorter path of contact and<br />

the product of contact stress and sliding velocity is the highest<br />

for this case of gearing compared to all other cases. Therefore,<br />

the lubricant between meshing surfaces is subjected to squeezing<br />

and breakdown of the lubricant film. This indicates a severe scoring<br />

effect. The extreme pressure and high sliding velocity caused<br />

ploughing of the material. In addition, dry sliding wear at the<br />

point of contact generates high friction and material removal<br />

from the surface acts as three-body wear and creates ploughing<br />

of the material, as shown in Figs. 3e and 3f. However, the cases<br />

of gearing with positive values of tooth number alterations are<br />

marginally scored compared to standard gearing. Surface examinations<br />

carried out by considering SEM microphotographs<br />

revealed better surface integrity for the cases of negative number<br />

of tooth alterations.<br />

CONCLUSIONS<br />

The analyses of maximum contact stress in altered tooth-sum<br />

gearing for a tooth-sum of 100 when altered by §4% have been<br />

studied. The magnitude of s max and morphological studies have<br />

been done for point B and point D. From the computational,<br />

experimental, and morphological analysis, the following conclusions<br />

are drawn:<br />

Better performance is obtained for negative alteration in<br />

tooth-sum gears compared to standard gearing. This is<br />

because the contact stress induced for negative alteration in<br />

tooth-sums of 96, 97, 98, and 99 is lower compared to the<br />

standard tooth-sum of 100. For positive alteration in toothsum<br />

the contact stress at points B 1 and B 2 is higher; in turn,<br />

standard gears perform better under these conditions for a<br />

25 pressure angle. Similarly, the analysis holds for a 20 <br />

pressure angle.<br />

It is proved that by a profile modification technique it is<br />

possible to trace the point of switchover of s max . In addition,<br />

it has design flexibility in gear design with respect to<br />

the range of contact ratio.


744 H. K. SACHIDANANDA ET AL.<br />

Downloaded by [Manipal University], [sachidananda H K] at 21:24 26 May 2015<br />

In a gear pair, altering the tooth number requires the use of<br />

a profile shift; moreover, these gears operate on an altered<br />

pressure angle. Thus, contact stress in these gears is influenced<br />

by changes due to altering the tooth numbers.<br />

Altering tooth-sum gearing using a profile shift has been<br />

used in design of gears with higher flexibility. This helps in<br />

designing gears with moderate material by utilizing its surface<br />

strength to a maximum extent. The analysis of maximum<br />

contact stresses in altered tooth-sum gearing helps in<br />

understanding the importance of a profile shift in design of<br />

gears for applications like rolling mills, etc. Altered toothsum<br />

gearing helps gear designers in exercising greater flexibility<br />

while designing gears.<br />

The SEM observations of the tooth surface show the importance<br />

of s max on surface damage. In addition, the morphology<br />

of the tooth specimen shows that microcracks are<br />

generated due to cyclic loading and will lead to pitting failure<br />

in the rolling direction.<br />

REFERENCES<br />

(1) Nabih, F. J., Cavoret, V., and Philippe, V. (2013), “Gear Tooth Pitting<br />

Modelling and Detection Based on Transmission Error Measurements,”<br />

European Journal of Computational Mechanics, 22(2–4), pp 106–119.<br />

(2) Ruben, D. C., Luis, J. A., Miguel, A., Diaz, A., and Jose, A. (2010),<br />

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in Helical Gears,” Wear, 249(3–4), pp 285–292.<br />

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Assessment in Spur Gears Using Lubricant Film Thickness and Vibration<br />

Signal Analysis,” Tribology Transactions, 58(2), pp 327–336.<br />

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(22) Marco, A. M., Fabio, K., Urbano, R., and Carlos, H. S. (2012), “The<br />

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the Wear of Spur Gears during Pitting Tests,” Journal of Braz. Society of<br />

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(24) Moldovan, Gh., Velicu, D., and Velicu, R. (2007), “On the Maximal<br />

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Besancon, France, June 18–27.<br />

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Contact Stresses in Altered Tooth-Sum Spur Gearing,” Journal of<br />

Applied Mechanical Engineering, 1(1), pp 1–5.<br />

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(27) Sheng, L. and Ahmet, K. (2011), “A Fatigue Model for Contacts under<br />

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Meshed Teeth’s Flanks along the Path of Contact for a Tooth Pair,”<br />

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