Q.Y. Deng et al.
Surface & Coatings Technology 358 (2019) 611–616
profiles of the wear tracks on the Cu and Co alloy discs are presented in
Fig. 2e. As shown, the depth of the wear track on the Cu disc is smaller
than that formed on the surface of Co alloy disc. This indicates that the
wear resistance of the Cu disc in the presence of the BSA solution is
better than that of Co alloy in the BSA solution. We infer that the “tribo-
layer” observed in the wear track of the Cu disc may have an important
influence on the wear resistance of Cu.
3.2. Raman and ATR-FTIR spectra of tribo-layer
In order to investigate the structure of the tribo-layers formed on the
wear tracks, micro-Raman spectra were acquired of the wear track
contact regions of the Al -Cu and Al -Co alloy tribo-pairs. The
Fig. 1. Schematic view of the tribology experiment.
2
O
3
2 3
O
results are shown in Fig. 3a and b. The Raman spectrum of the tribo-
layer formed inside wear track of the Cu disc (black area in Fig. 2a,
denoted with a yellow circle) showed strong Raman activity with a D
dimensions Φ 10 mm × 1.5 mm, were polished to a surface roughness
) of ~10 nm. After polishing, the discs were ultrasonically cleaned in
acetone and then in alcohol for 10 min each before being subjected to
wear testing.
Wear tests were performed using a ball-on-disc reciprocating trib-
ometer (CSEM, Switzerland) under a load of 1 N for 100,000 cycles.
2 3
Al O balls of 6 mm diameter were used to create the friction pairs
against the Co alloy and Cu discs in a total volume of 50 mL bovine
serum albumin solution (BSA solution, composition: BSA 20 mg/mL,
NaCl: 9 mg/mL, EDTA: 2 mg/mL, sorbic acid: 0.2 mg/mL) at a room
temperature of around 25 °C. The length of the wear track was about
(R
q
−1
−1
peak around 1380 cm
and a G peak around 1580 cm
(shown in
Fig. 3a). This indicated that the structure of the tribo-layer formed in-
side wear track of the Cu disc was comprised of graphite-like materials;
i.e., that it was a carbonaceous film. On the other hand, the Raman
spectrum of the wear track on the Co alloy (area in Fig. 2b, denoted
with a yellow circle) showed no Raman activity, similar to that of the
dried BSA (shown in Fig. 3b). That indicated that, under the conditions
employed in this work, the friction between alumina and the Co alloy
did not transform the BSA molecules in the wear track into a carbo-
naceous film.
6
mm and the sliding frequency was 1 Hz. The schematic view of the
tribology experiment setup is shown in Fig. 1.
In order to identify changes in the bonding of the BSA molecules
during friction, the Infra-Red spectra of the tribo-layers formed inside
wear tracks of the Cu and Co alloy discs were collected using
Attenuated Total Reflection Fourier Transform Infra-Red (ATR-FTIR)
spectroscopy. Dried BSA used as a control. The results, presented in
Fig. 3c and d, show that dried BSA contained two main peaks: the
2.2. Characterization of BSA adsorption
The adsorption of fluorescein isothiocyanate (FITC) modified BSA
molecules onto the wear track was determined from fluorescein images
captured using a Fluoresce Microscope (IX51, Olympus, Japan).
−
1
−1
amide I band at 1645 cm and the amide II band at 1530 cm . Fig. 3c
shows that the spectrum of outside wear track on the Cu disk is similar
to that of the dried BSA. The spectrum of the tribo-film formed inside
wear track on the Cu disk, however, was obviously different from that
2.3. Morphology of the wear track
−
1
of the dried BSA. A new absorption peak appears at 1600 cm , which
represents the formation of a eC]Ce bond (shown in Fig. 3c). This
clearly indicates that the structure of tribo-layer inside wear track on
the Cu disk was different to that of dried BSA, likely due to the dena-
turing of the BSA molecules under the cyclical shear force between the
alumina ball and the Cu disk to form the carbonaceous film. The
spectrum of tribo-layer formed inside wear track on the Co alloy (shown
After the wear tests, the morphology of wear tracks and spots were
investigated using an optical microscope (AX10, ZEISS, Germany). The
profile of the wear tracks was determined using a profilometer (XP2,
AMBIOS, USA).
2
.4. Characterization of the structure of tribological layer
−1
in Fig. 3d) showed a mere blue-shift of the amide I (from 1645 cm to
A Raman microscope (λ = 532 nm, InVia Raman Microscope,
−1
−1
−1
1
657 cm ) and amide II (from 1530 cm to 1546 cm ) bands. This
RENISHAW, Britain) and an Attenuated Total Reflection Fourier
Transform Infra-Red (ATR-FTIR, Nicolet 8500, USA) were used to in-
vestigate the structure of tribo-layer formed on the wear track. An
Electron Energy Loss Spectrometer (EELS, JEOL 2100F, Japan) and
Time-of-Flight Secondary Ion Mass Spectrometer (TOF-SIMS, PHI
TRIFT III, Japan) were used to characterize the structure of the tribo-
layer formed on the surface of wear spot.
indicated a change in the highly-ordered structure of BSA upon ad-
sorption onto the Co alloy.
3.3. TOF-SIMS of tribo-layer
Time of Flight Secondary Ion Mass Spectrometry (TOF-SIMS) is a
versatile method to reveal, with high resolution, the chemical char-
acteristics of a surface. The TOF-SIMS spectra and mapping of the tribo-
3. Results
2 3
layers from inside the wear spot on the Al O after contact with the
different metals, as well as from the areas surrounding the wear spot
(i.e., outside the wear spot) are shown in Fig. 4.
3.1. Surface morphology and profile of wear track
As shown in Fig. 4a, the SIMS spectrum of the tribo-layer obtained
The microscope images of the wear tracks on the discs and the as-
2 3
from inside the wear spot of the Al O ball after wear contact with the
sociated wear spots on the Al
2
O
3
balls in contact with the respective
Co alloy in the BSA solution is similar to that of obtained from outside
the wear spot. The mapping of the wear spot of the alumina-Co alloy
pair (Fig. 4b) also shows that there is no obvious difference between the
inside wear spot and outside wear spot. This reveals that the chemical
surfaces, as well as the profiles of wear tracks are shown in Fig. 2. After
the wear test experiments with alumina balls in the BSA solution, ob-
vious furrows appeared on the surfaces of the metal discs (Fig. 2a and
b). Notably, a ‘black tribo-layer’ appeared in the wear track of the Cu
disc (Fig. 2a) that was absent in the wear track of the Co alloy (Fig. 2b).
The microscope images of the wear spot on the alumina worn with the
Cu and Co alloy discs are shown in Fig. 2c and d, respectively. The
2 3
nature of tribo-layer appearing on the wear spot of the Al O -Co alloy is
similar to that of the materials outside of the wear spot, indicating
further that the BSA molecules were not denatured or transformed into
a carbonaceous layer under friction between the alumina and the Co
612