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Alexandria Engineering Journal , Vol. (43) (2004), No. 5, 615-619 615
© Faculty of Engineering Alexandria University, Egypt.
A new reciprocating tribometer for wear testing under different
fluctuating loading conditions
A. Abdelbary, M. N. Abouelwafa, I. M. El Fahham and A. I. Gomaa
Mechanical Eng. Dept., Faculty of Eng., Alexandria University, Alexandria, Egypt
A new reciprocating testing machine was designed and constructed to perform wear tests
under constant and fluctuating loading conditions at a constant sliding speed for most of its
stroke. The tribometer has the facility of changing the amplitude, mean load and the
frequency of loading cycle. The wear tests can, also, be conducted under dry or wet
conditions. The influence of loading mode on the wear behavior of Nylon 66 sliding against
stainless steel in dry conditions was investigated on this test rig. The polymer was tested
under constant and fluctuating loading conditions at two different loads and at three
frequencies. Results suggested that under cyclic loading condition the polymer shows a
significant increase in wear factor than those found under constant loads. The frequency of
load cycle, also, has a pronounced influence on the wear behavior under cyclic load.
.
.
.
.
.
Keyword: Wear, Tribometer, Cyclic load
1. Introduction
The need of investigating the effect of
dynamic loading associated to many practical
applications, on the wear behavior was the
motive to develop a satisfactory laboratory
tribometer, which is able to perform such
tests. In many previous works [1, 2, 3] the
wear tests were conducted using a
reciprocating wear machine where the polymer
pin was subjected to a constant load and
slides on a reciprocating bed, which was
driven by a cam mechanism. In such configu-
ration, the counterface reciprocated with a
variable speed having a pre-determined
average value. In order to study the influence
of variable load on the wear of Ultra-High
Molecular Weight Polyethylene (UHMWPE) [4],
a similar tribometer of six stations was used.
The time dependent nature of loading was
monitored using a load cell in the loading arm
and could be controlled to give an approxi-
mate square wave form. Another system was
developed [5] which incorporates a sine cam
mechanical system to generate an alternating
sine curve load at the wear surface to simulate
the loading produced by masticatory process.
The effect of cyclic load on the wear
behavior of polymers has previously been
detected as a form of surface fatigue wear [4,
6] where a significant increase of 30% in the
wear of UHMWPE was observed when testing
the polymer under cyclic loading condition.
The same trend was, also, found in other work
[7]. The cyclic load has two major effects on
polymeric wear; first, the loading – unloading
cycle is responsible for creating a highly
subsurface stressed regions which in turn,
after a number of loading cycles, initiating
subsurface cracks [7,8]. The microscopic
crack, then, grows a small amount during the
peak load of each cycle [9]. Subsurface crack
propagation may well have accelerated the
failure and removal of material from the highly
strained polymer peaks, hence greatly increas-
ing the polymer wear [10]. Second the thermal
A. Abdelbary et al. / Wear testing
616 Alexandria Engineering Journal, Vol. 43, No. 5, September 2004
effect of the loading frequency on the dynamic
mechanical properties of the bulk polymer.
Generally, the effect of loading frequency is to
increase the temperature of the bulk polymer,
which in turn causes a decrease in the shear
modulus, G, and in the fatigue life specially at
high frequencies [9]. Although the frequency
effect is small at low frequencies but the
increase in the temperature of specimen due
to friction will magnifies the frequency effect
[11]. The mutual effect of the temperature and
applied frequency is to soften the polymer and
decrease its modulus, which leads to increase
the fatigue wear.
In the present work a new reciprocating
tribometer was designed and constructed to
study the effect of different fluctuating loading
conditions on the wear of polymers. The tri-
bometer has the capacity of testing the wear
behavior of materials under static or fluctuat-
ing load in dry or lubricated environment. The
amplitude, mean and frequency of the cyclic
load are controllable. To eliminate the effect of
speed variations on wear, the new tribometer
has the advantage of performing the tests at
constant speed of the counterface for most of
the stroke.
2. Tribometer
It consists of a 2.2 kW motor (2) drives the
chain mechanism (3), using a gearbox to
reduce the speed to 31.5 rpm. This mecha-
nism is used to drive the carriage (5) by
replacing one of the pins of the chain by a
special pin with extra length to project from
the side of the chain. A small deep groove ball
bearing is mounted at the end of this pin and
rolls inside a U-beam guide (4), which is
welded at the bottom of the carriage. With
such configuration the carriage reciprocates
with constant linear speed for 80%of its, 310-
mm, stroke. The sliding speed is selected to be
0.25 m/s. The carriage is divided into six
separated channels to promote the activation
of maximum number of independent tests at
the same time. The counterfaces are fixed to
the channels at 30-mm depth to enable both
dry and lubricated tests. The fluctuated load
is generated by a special loading system,
which consists of a set of six eccentric
replicable cams (6). The cam follower (7)
transmits the displacement of the cam
rotation to a vertical compression spring (8),
which transmits the generated force to the pin
holder (9). The spring is mounted on a
movable controlled seat (10) that can be used
to adjust the initial deflection of the spring.
The loading cycle due to this arrangement has
a sinusoidal form. The cam shaft is driven by
a 0.74 kW motor with a second gearbox (11)
giving three different frequencies.
Fig. 1. General lay out of the wear testing M/C: (1) machine frame; (2) 2.2 kW motor; (3) chain drive mechanism; (4) U-
beam guide; (5) carriage; (6) eccentric cam; (7) cam follower; (8) spring; (9) pin holder; (10) movable spring seat; (11) 0.74
kW motor.
A. Abdelbary et al. / Wear testing
Alexandria Engineering Journal, Vol. 43, No. 5, September 2004 617
Fig. 2. Wear testing M/C.
The amplitudes and means of the cyclic
loads can be controlled by changing the cams
and/or springs. Other forms of loading cycle
can be, also, applied using different cam
shapes. Constant load tests can be performed
separately by switching off the 0.74 kW motor
and applying a specific constant deflection to
the spring. The generated load can be
calibrated using a load cell. The wear rate of
test specimens is determined from measure-
ment of weight or volume loss. Fig. 1&2
represent a general lay out of the tribometer.
3. Tests
Wear tests were carried out using Nylon 66
wear pins machined from solid bar into a
cylindrical shape with one end machined to a
truncated cone of 80o included angle,
presenting an initial wear face of 16-20 mm2.
The counterfaces were prepared from stainless
steel plates ground to provide a surface with a
center line average (Ra) value of about 0.5 µm.
These sheets presented a rectangular wear
face of 330 x 30 mm. Role of control pins and
standard test procedures [3] were taken into
consideration. The Wear Factor (WF) is deter-
mined as WF = Volume loss/ Sliding distance
X Applied load.
4. Results
First, the polymer was tested under two
different constant loads 70N, 90N in a dry
sliding condition. Then, the polymer was
tested under cyclic loading at two different
means; 70N and 90N while the amplitude of
the cycle was adjusted to 35N. The tests were
performed at three different frequencies 0.38,
0.7 and 1.38 Hz. Table 1 represents the wear
results of these tests. Figs. 3 and 4 show the
variation of the worn volume in mm3 with the
sliding distance in km.
Fig. 3. Variation of Nylon 66 volume loss with sliding
distance after 100 km, P (constant, mean) = 70 N.
Fig. 4. Variation of Nylon 66 volume loss with sliding
distance after 100 km, P (constant, mean) = 90 N.
A. Abdelbary et al. / Wear testing
618 Alexandria Engineering Journal, Vol. 43, No. 5, September 2004
Table 1
Wear results for constant and cyclic load testes
a- Constant Load Tests
Test
No.
f
Hz
P
N.
X
km
V
mm3
WF
x10-6
mm3/
N.m
1 - 70 95 39 5.3
2 - 90 95 66 6.3
b- Cyclic Load Tests
3 0.38 70* 133 70 7.7
4 90* 133 115 10
5 70* 100 62 7.5
6
0.70
90* 100 132 15
7 70* 100 73 10.6
8
1.38
90* 100 153 17
* Mean of the load cycle
The results show that the cyclic load
produces more than 40% increase in the wear
factor. This implies that the time dependent
nature of the load in the cyclic load tests
generates higher wear rates. The results also
indicate that the increase in wear factor is
influenced by the frequency of the loading
cycle.
5. Discussion and conclusion
The results of tests at the three examined
frequencies, 0.38, 0.7 and 1.38 Hz, indicate
that the wear factor increases significantly
with increasing the cyclic frequency at the two
ranges of mean loads. As mentioned earlier,
the existence of the time dependence nature of
loading increases the wear factor than its
value under constant load of the same magni-
tude as the mean load. The fatigue wear
process seems to be the dominant mechanism
of wear. Generally, increasing frequency pro-
duces an increase in temperature of the bulk
polymer leading to a decrease in mechanical
properties and fatigue safe-life [9, 12].
The dynamic fatigue properties of polymer
in bulk often involve thermal effects attribut-
able to heat build – up within the polymer and
are thus very sensitive to the frequency and
form of the applied cyclic stress [13]. This
suggests that the increase in wear factors
found when increasing frequency is due to the
effect of frequency on the fatigue and me-
chanical characteristics of the bulk polymer.
A useful observation is that there is a
significant increase in the total worn volume
due to the applied frequency. The need of such
remark is that in many mechanical and
medical polymeric applications, the total
volume loss may has a superior priority in
calculating the life time of the component
rather than the wear factor.
The presented tribometer has been demon-
strated as a good testing instrument for
particular applications where investigating the
wear behavior under fluctuating loading is
required. The tribometer has the capacity to
perform wear tests under constant or cyclic
loading conditions. Also, it has the ability to
change the amplitude, mean load and fre-
quency of the loading cycle. The wear tests
that have been conducted on the tribometer
indicated that;
Under cyclic loading condition, in which
the mean of the load cycle equals in magni-
tude to the constant load, Nylon 66 shows a
significant increase, for more than 40%, in
wear factors than those found under constant
loads. This can be explained as that the fluc-
tuating load generally increases the fatigue
effect on wear that existed under constant
loading condition.
Increasing the frequency of load cycle
leading to an increase in wear factor as well as
in total volume loss. Results indicated a linear
relationship between frequency and both wear
factors and worn volume.
References
[1] P.S.M. Barbour, D.C. Barton and J.
Fisher, “The Influence of Contact Stress
on the Wear of UHMWPE for Total
Replacement Hip Prostheses”, Wear, Vol.
181-183, pp. 250-257 (1995).
[2] D. Dowson, J.M. Challen, K. Holmes and
Atkenson J.R., “The Wear of Non-Metallic
Materials”, Paper IV, Proceeding of the 3rd
Leeds-Lyon Symposium on Tribology,
September (1976).
[3] K. reber, J.R. Atkenson and D. Dowson,
“The Mechanisms for Nylon 66” Paper II,
Proceeding of the 3rd Leeds-Lyon
Symposium on Tribology, September
(1976).
[4] J. Fisher, “Wear of UHMWPE in Total
Artificial Joints”, Current Orthopedics,
Vol. 8, pp. 164-196 (1994).
A. Abdelbary et al. / Wear testing
Alexandria Engineering Journal, Vol. 43, No. 5, September 2004 619
[5] X. Hu, E. Harringlon, P.M. Marquis and
A.C. Shortall, “The Influence of Cyclic
Loading on The Wear of a Dental
Composite”, Biomaterials, Vol. 20 (10) pp.
907-912 (1999).
[6] P.S.M. Barbour, M.H. Stone, J. Fisher, “A
Study of The Wear Resistance of Three
Types of Clinically Applied UHMWPE for
Total Replacement Hip Prostheses”,
Biomaterials, Vol. 20, pp. 2101-2106
(1999).
[7] G.W. Blumm, S. Walker, A. Joshi and K.
Hardinge, “The Dominance of Cyclic
Sliding in Producing Wear in total Knee
Replacements”, Clin. Orthop., December
(1991).
[8] L.H. Mair, “Wear in Dentistry – Current
Terminology”, J. Dent., Vol. 20, pp.140–
144 (1992).
[9] K. Gupta Rakesh, Polymer and Composite
Rheology, Marcel Dekker Inc, (ISBN: 0-
8247-9922-4) (2000).
[10] A.U.J. Yap, S.H. Teoh and C.L. Chew,
“Effect of Cyclic Loading on Occlusal
Contact Area Wear of Composite
Restoratives”, Dental Materials, Vol. 18
(2), pp. 149-158 (2002).
[11] V. Zivlar, “Plastics Polymers”, Vol. 39, p.
328 (1971).
[12] C. Osgood Carl, Fatigue Design,
Pergamon Press, (ISBN: 0-08-026167-1).
[13] A.E. Hollander, J.K. Lancaster, “An
Application of Topographical Analysis to
The Wear of Polymers”, Wear, Vol. 25, pp.
155-170 (1973).
Received December 13, 2003
Accepted March 20, 2004

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A new reciprocating tribometer for wear testing under different

  • 1. Alexandria Engineering Journal , Vol. (43) (2004), No. 5, 615-619 615 © Faculty of Engineering Alexandria University, Egypt. A new reciprocating tribometer for wear testing under different fluctuating loading conditions A. Abdelbary, M. N. Abouelwafa, I. M. El Fahham and A. I. Gomaa Mechanical Eng. Dept., Faculty of Eng., Alexandria University, Alexandria, Egypt A new reciprocating testing machine was designed and constructed to perform wear tests under constant and fluctuating loading conditions at a constant sliding speed for most of its stroke. The tribometer has the facility of changing the amplitude, mean load and the frequency of loading cycle. The wear tests can, also, be conducted under dry or wet conditions. The influence of loading mode on the wear behavior of Nylon 66 sliding against stainless steel in dry conditions was investigated on this test rig. The polymer was tested under constant and fluctuating loading conditions at two different loads and at three frequencies. Results suggested that under cyclic loading condition the polymer shows a significant increase in wear factor than those found under constant loads. The frequency of load cycle, also, has a pronounced influence on the wear behavior under cyclic load. . . . . . Keyword: Wear, Tribometer, Cyclic load 1. Introduction The need of investigating the effect of dynamic loading associated to many practical applications, on the wear behavior was the motive to develop a satisfactory laboratory tribometer, which is able to perform such tests. In many previous works [1, 2, 3] the wear tests were conducted using a reciprocating wear machine where the polymer pin was subjected to a constant load and slides on a reciprocating bed, which was driven by a cam mechanism. In such configu- ration, the counterface reciprocated with a variable speed having a pre-determined average value. In order to study the influence of variable load on the wear of Ultra-High Molecular Weight Polyethylene (UHMWPE) [4], a similar tribometer of six stations was used. The time dependent nature of loading was monitored using a load cell in the loading arm and could be controlled to give an approxi- mate square wave form. Another system was developed [5] which incorporates a sine cam mechanical system to generate an alternating sine curve load at the wear surface to simulate the loading produced by masticatory process. The effect of cyclic load on the wear behavior of polymers has previously been detected as a form of surface fatigue wear [4, 6] where a significant increase of 30% in the wear of UHMWPE was observed when testing the polymer under cyclic loading condition. The same trend was, also, found in other work [7]. The cyclic load has two major effects on polymeric wear; first, the loading – unloading cycle is responsible for creating a highly subsurface stressed regions which in turn, after a number of loading cycles, initiating subsurface cracks [7,8]. The microscopic crack, then, grows a small amount during the peak load of each cycle [9]. Subsurface crack propagation may well have accelerated the failure and removal of material from the highly strained polymer peaks, hence greatly increas- ing the polymer wear [10]. Second the thermal
  • 2. A. Abdelbary et al. / Wear testing 616 Alexandria Engineering Journal, Vol. 43, No. 5, September 2004 effect of the loading frequency on the dynamic mechanical properties of the bulk polymer. Generally, the effect of loading frequency is to increase the temperature of the bulk polymer, which in turn causes a decrease in the shear modulus, G, and in the fatigue life specially at high frequencies [9]. Although the frequency effect is small at low frequencies but the increase in the temperature of specimen due to friction will magnifies the frequency effect [11]. The mutual effect of the temperature and applied frequency is to soften the polymer and decrease its modulus, which leads to increase the fatigue wear. In the present work a new reciprocating tribometer was designed and constructed to study the effect of different fluctuating loading conditions on the wear of polymers. The tri- bometer has the capacity of testing the wear behavior of materials under static or fluctuat- ing load in dry or lubricated environment. The amplitude, mean and frequency of the cyclic load are controllable. To eliminate the effect of speed variations on wear, the new tribometer has the advantage of performing the tests at constant speed of the counterface for most of the stroke. 2. Tribometer It consists of a 2.2 kW motor (2) drives the chain mechanism (3), using a gearbox to reduce the speed to 31.5 rpm. This mecha- nism is used to drive the carriage (5) by replacing one of the pins of the chain by a special pin with extra length to project from the side of the chain. A small deep groove ball bearing is mounted at the end of this pin and rolls inside a U-beam guide (4), which is welded at the bottom of the carriage. With such configuration the carriage reciprocates with constant linear speed for 80%of its, 310- mm, stroke. The sliding speed is selected to be 0.25 m/s. The carriage is divided into six separated channels to promote the activation of maximum number of independent tests at the same time. The counterfaces are fixed to the channels at 30-mm depth to enable both dry and lubricated tests. The fluctuated load is generated by a special loading system, which consists of a set of six eccentric replicable cams (6). The cam follower (7) transmits the displacement of the cam rotation to a vertical compression spring (8), which transmits the generated force to the pin holder (9). The spring is mounted on a movable controlled seat (10) that can be used to adjust the initial deflection of the spring. The loading cycle due to this arrangement has a sinusoidal form. The cam shaft is driven by a 0.74 kW motor with a second gearbox (11) giving three different frequencies. Fig. 1. General lay out of the wear testing M/C: (1) machine frame; (2) 2.2 kW motor; (3) chain drive mechanism; (4) U- beam guide; (5) carriage; (6) eccentric cam; (7) cam follower; (8) spring; (9) pin holder; (10) movable spring seat; (11) 0.74 kW motor.
  • 3. A. Abdelbary et al. / Wear testing Alexandria Engineering Journal, Vol. 43, No. 5, September 2004 617 Fig. 2. Wear testing M/C. The amplitudes and means of the cyclic loads can be controlled by changing the cams and/or springs. Other forms of loading cycle can be, also, applied using different cam shapes. Constant load tests can be performed separately by switching off the 0.74 kW motor and applying a specific constant deflection to the spring. The generated load can be calibrated using a load cell. The wear rate of test specimens is determined from measure- ment of weight or volume loss. Fig. 1&2 represent a general lay out of the tribometer. 3. Tests Wear tests were carried out using Nylon 66 wear pins machined from solid bar into a cylindrical shape with one end machined to a truncated cone of 80o included angle, presenting an initial wear face of 16-20 mm2. The counterfaces were prepared from stainless steel plates ground to provide a surface with a center line average (Ra) value of about 0.5 µm. These sheets presented a rectangular wear face of 330 x 30 mm. Role of control pins and standard test procedures [3] were taken into consideration. The Wear Factor (WF) is deter- mined as WF = Volume loss/ Sliding distance X Applied load. 4. Results First, the polymer was tested under two different constant loads 70N, 90N in a dry sliding condition. Then, the polymer was tested under cyclic loading at two different means; 70N and 90N while the amplitude of the cycle was adjusted to 35N. The tests were performed at three different frequencies 0.38, 0.7 and 1.38 Hz. Table 1 represents the wear results of these tests. Figs. 3 and 4 show the variation of the worn volume in mm3 with the sliding distance in km. Fig. 3. Variation of Nylon 66 volume loss with sliding distance after 100 km, P (constant, mean) = 70 N. Fig. 4. Variation of Nylon 66 volume loss with sliding distance after 100 km, P (constant, mean) = 90 N.
  • 4. A. Abdelbary et al. / Wear testing 618 Alexandria Engineering Journal, Vol. 43, No. 5, September 2004 Table 1 Wear results for constant and cyclic load testes a- Constant Load Tests Test No. f Hz P N. X km V mm3 WF x10-6 mm3/ N.m 1 - 70 95 39 5.3 2 - 90 95 66 6.3 b- Cyclic Load Tests 3 0.38 70* 133 70 7.7 4 90* 133 115 10 5 70* 100 62 7.5 6 0.70 90* 100 132 15 7 70* 100 73 10.6 8 1.38 90* 100 153 17 * Mean of the load cycle The results show that the cyclic load produces more than 40% increase in the wear factor. This implies that the time dependent nature of the load in the cyclic load tests generates higher wear rates. The results also indicate that the increase in wear factor is influenced by the frequency of the loading cycle. 5. Discussion and conclusion The results of tests at the three examined frequencies, 0.38, 0.7 and 1.38 Hz, indicate that the wear factor increases significantly with increasing the cyclic frequency at the two ranges of mean loads. As mentioned earlier, the existence of the time dependence nature of loading increases the wear factor than its value under constant load of the same magni- tude as the mean load. The fatigue wear process seems to be the dominant mechanism of wear. Generally, increasing frequency pro- duces an increase in temperature of the bulk polymer leading to a decrease in mechanical properties and fatigue safe-life [9, 12]. The dynamic fatigue properties of polymer in bulk often involve thermal effects attribut- able to heat build – up within the polymer and are thus very sensitive to the frequency and form of the applied cyclic stress [13]. This suggests that the increase in wear factors found when increasing frequency is due to the effect of frequency on the fatigue and me- chanical characteristics of the bulk polymer. A useful observation is that there is a significant increase in the total worn volume due to the applied frequency. The need of such remark is that in many mechanical and medical polymeric applications, the total volume loss may has a superior priority in calculating the life time of the component rather than the wear factor. The presented tribometer has been demon- strated as a good testing instrument for particular applications where investigating the wear behavior under fluctuating loading is required. The tribometer has the capacity to perform wear tests under constant or cyclic loading conditions. Also, it has the ability to change the amplitude, mean load and fre- quency of the loading cycle. The wear tests that have been conducted on the tribometer indicated that; Under cyclic loading condition, in which the mean of the load cycle equals in magni- tude to the constant load, Nylon 66 shows a significant increase, for more than 40%, in wear factors than those found under constant loads. This can be explained as that the fluc- tuating load generally increases the fatigue effect on wear that existed under constant loading condition. Increasing the frequency of load cycle leading to an increase in wear factor as well as in total volume loss. Results indicated a linear relationship between frequency and both wear factors and worn volume. References [1] P.S.M. Barbour, D.C. Barton and J. Fisher, “The Influence of Contact Stress on the Wear of UHMWPE for Total Replacement Hip Prostheses”, Wear, Vol. 181-183, pp. 250-257 (1995). [2] D. Dowson, J.M. Challen, K. Holmes and Atkenson J.R., “The Wear of Non-Metallic Materials”, Paper IV, Proceeding of the 3rd Leeds-Lyon Symposium on Tribology, September (1976). [3] K. reber, J.R. Atkenson and D. Dowson, “The Mechanisms for Nylon 66” Paper II, Proceeding of the 3rd Leeds-Lyon Symposium on Tribology, September (1976). [4] J. Fisher, “Wear of UHMWPE in Total Artificial Joints”, Current Orthopedics, Vol. 8, pp. 164-196 (1994).
  • 5. A. Abdelbary et al. / Wear testing Alexandria Engineering Journal, Vol. 43, No. 5, September 2004 619 [5] X. Hu, E. Harringlon, P.M. Marquis and A.C. Shortall, “The Influence of Cyclic Loading on The Wear of a Dental Composite”, Biomaterials, Vol. 20 (10) pp. 907-912 (1999). [6] P.S.M. Barbour, M.H. Stone, J. Fisher, “A Study of The Wear Resistance of Three Types of Clinically Applied UHMWPE for Total Replacement Hip Prostheses”, Biomaterials, Vol. 20, pp. 2101-2106 (1999). [7] G.W. Blumm, S. Walker, A. Joshi and K. Hardinge, “The Dominance of Cyclic Sliding in Producing Wear in total Knee Replacements”, Clin. Orthop., December (1991). [8] L.H. Mair, “Wear in Dentistry – Current Terminology”, J. Dent., Vol. 20, pp.140– 144 (1992). [9] K. Gupta Rakesh, Polymer and Composite Rheology, Marcel Dekker Inc, (ISBN: 0- 8247-9922-4) (2000). [10] A.U.J. Yap, S.H. Teoh and C.L. Chew, “Effect of Cyclic Loading on Occlusal Contact Area Wear of Composite Restoratives”, Dental Materials, Vol. 18 (2), pp. 149-158 (2002). [11] V. Zivlar, “Plastics Polymers”, Vol. 39, p. 328 (1971). [12] C. Osgood Carl, Fatigue Design, Pergamon Press, (ISBN: 0-08-026167-1). [13] A.E. Hollander, J.K. Lancaster, “An Application of Topographical Analysis to The Wear of Polymers”, Wear, Vol. 25, pp. 155-170 (1973). Received December 13, 2003 Accepted March 20, 2004