Functionalized and fully characterized graphene-based lubricant additives are potential 2D materials for energy-efficient tribological applications in machine elements, especially at macroscopic contacts. Two different reduced graphene oxide (rGO) derivatives, terminated by hydroxyl and epoxy-hydroxyl groups, were prepared and blended with two different molecular weights of polyethylene glycol (PEG) for tribological investigation. Epoxy-hydroxyl-terminated rGO dispersed in PEG showed significantly smaller values of the friction coefficient. In this condition, PEG chains intercalate between the functionalized graphene sheets, and shear can take place between the PEG and rGO sheets. However, the friction coefficient was unaffected when hydroxyl-terminated rGO was coupled with PEG. This can be explained by the strong coupling between graphene sheets through hydroxyl units, causing the interaction of PEG with the rGO to be non- effective for lubrication. On the other hand, antiwear properties of hydroxyl-terminated rGO were significantly enhanced compared to epoxy-hydroxyl functionalized rGO due to the integrity of graphene sheet clusters.
Lubricants reduce friction between contacting surfaces and thus increase the energy efficiency of moving machine components. Several remarkable properties of graphene-oxide/reduced graphene-oxide (GO/rGO) make it an effective solid additive for liquid lubricants1,2,3,4,5. These include low shear strength, high yield strength, chemical compatibility for dispersion in polar lubricants, and high thermal conductivity and an ecofriendly composition5,6. However, toxicity of graphene and related risks for the health cannot be ignored7. A small amount of GO/rGO is capable of effective lubrication due to high surface to volume ratio, effective inter-sheet shearing and sufficient oxygen functionality making GO/rGO compatible for dispersion in polar liquid lubricants1,3,8. The layered lattice structure is unique for reducing inter-sheet shear resistance and has shown low friction coefficients combined with the high strength of the graphene sheets6,9. Optimization of oxygen functionality in GO/rGO is an important aspect for preserving the chemical stability of the structure while providing sustainable covalent/noncovalent interactions with the lubricant. Lubrication enhancement by GO/rGO additives was described by the formation of low-shear-strength graphene tribofilm by adsorption to metal surfaces1,2,10. However, the lubrication mechanism was effective also without forming mechanically stable graphene tribofilms within the sliding interfaces11. In this case, lubrication acts through shearing of the physisorbed functionalized graphene sheets under the contact.
The properties of the liquid lubricant, including molecular weight and polarity, are also decisive for lubrication12,13. High molecular weight and high viscosity are important for high wear resistance while forming a high strength boundary tribofilm. However, shear resistance of the boundary film may increase the friction coefficient. Therefore, optimization of shear properties of the lubricant through the modification of viscosity is one of the most important criteria for effective lubrication. The dispersion of GO/rGO additives in the blends can assist in such optimization. For example, GO was also used as additive to enhance the antiwear properties of a mineral oil using a dispersant2. The dispersion of GO/rGO depends on the polarity of the lubricant and the functional groups of the GO/rGO. GO/rGO structures have a larger energy corrugation and higher shear strength than graphene due to localized electronic charge on the oxygen functionalities. These intrinsic properties degrade the tribological properties of GO/rGO compared to graphene. However, dispersion of graphene is not possible in hydrophilic lubricants due to the high cohesive energy, which makes the use of graphene for tribological applications unfeasible. The electrostatic and hydrogen bond interactions of GO/rGO and the dispersive medium were found to play a dominant role in its dispersion stability14,15,16. This is also related to the specific oxygen functionalization of GO/rGO. For example, a large lateral force is dominated by an interlayer hydrogen-bonded epoxy-hydroxyl coupling in GO/rGO. This leads to dissipation of frictional energy, manifested by higher adhesion and high strength of sliding resistance17. It should be noted that epoxy-epoxy and hydroxyl-hydroxyl interactions are weaker than epoxy-hydroxyl ones. The number of epoxide and hydroxyl groups in GO depends on the extent of oxidation of graphene. Higher oxidation of graphene may therefore induce more hydrogen bonds between epoxide and hydroxyl groups, indicating high binding energy and, consequently, higher shear strength17. However, the effects of hydroxyl and epoxy-hydroxyl GO functionalization on the micro/macrotribological properties of GO/rGO blended with a liquid lubricant have not been studied yet.
In this work, hydroxyl- and epoxy-hydroxyl-functionalized rGO samples were chemically prepared by controlled oxidation of bulk graphite powder followed by reduction. For simplicity, the hydroxyl- and epoxy-hydroxyl-functionalized rGO samples were designated as rGO1 and rGO2, respectively. The synthesized rGO was subjected to various microscopic and spectroscopic characterization techniques for detailed morphological, structural and chemical characterizations. The friction and wear properties of the rGO additives were investigated in two different molecular weights of polyethylene glycol (PEG). PEG is nonhazardous and it chemically interacts with rGO. Both rGO and PEG contain polar groups which provide effective dispersion stability through hydrogen bonding. Moreover, PEG is widely used in biomedical applications for reducing the friction and wear of knee joints18,19, but the use of rGO as blend additive to PEG for biomedical applications needs to be thoroughly investigated in term of safety7. The interaction mechanism of hydroxyl-hydroxyl and epoxy-hydroxyl terminated rGO with PEG were investigated. These interactions were used to interpret the friction and wear behavior of these rGO additives. The wear tracks were characterized by micro-Raman spectroscopy and X-ray photoelectron spectroscopy to reveal the friction and wear mechanism.
Results and Discussion
Chemical and structural characterization of rGO
Well-resolved diffraction peaks of the (0 0 2) plane were observed in rGO1 and rGO2 at 2θ of 21.5° and 24.8°, respectively, indicating lattice spacing of 0.4 and 0.36 nm in rGO1 and rGO2, respectively (Fig. 1). In crystalline graphite, this value is 0.34 nm and the increase in lattice spacing in rGO indicates the presence of oxygen functional groups. The broad peak in these samples correspond to few layers of rGO sheets in the particles20, indicating the presence of multilayer domains along with few mono-layered rGO sheets. The shoulder at 2θ of 16.5° in rGO2 is related to intercalation of oxygen groups or water molecules causing increase in interlayer spacing to 0.53 nm21. A small diffraction peak at 2θ of 47.8° is related to the (1 0 2) plane of rGO structure.
The folded and corrugated morphology of the rGO sheets is shown in the low resolution TEM images (Fig. 2a and c). The surface corrugation is related to localized intrinsic strain due to loading of oxygen functional groups at the graphene sheets6,22. Well-aligned graphene/rGO sheets are evident in the high resolution TEM images (Fig. 2b and d). The AFM analysis showed rGO sheets of hundreds of nm in lateral dimensions and thicknesses of approximately 1 nm (Fig. 2e and f). This indicates that rGO contains few monolayers of graphene sheets in each particle, demonstrating the integrity of the graphene planes after the chemical treatments.
In XPS, the C 1 s peak of both rGO samples was de-convoluted into three chemically shifted segments, designated CX, CY and CZ at binding energies of 284.3, 285.8 and 288.2 eV, respectively (Fig. 3a and c)20,23. Segment CX was assigned to non-oxygenated carbon of C–C/C–H representing the graphene structure23. This fact is well supported by XRD and TEM analysis. Segment CY described the interaction of carbon atoms with oxygen in either hydroxyl (C–OH) or epoxide (C–O) functional groups. The carbonyl (>C = O) segment was identified as CZ, which relates to carbon functionalized in COOH. The intensity of the carbonyl peak (CZ) was higher in rGO2 than in rGO1 samples, indicating a higher content of COOH complexes. This functional group is typically located at the edges of the graphene sheets, while the epoxy group evolves at the basal plane of the graphene sheets creating the in-plane defects and disorder22.
The ratio of the CX peak intensity to the sum of the (CY + CZ) peak intensities was smaller in rGO2 (0.72) than in rGO1 (0.84), indicating higher content of oxygen functionalities in rGO2. This is presumably associated with the higher concentration of the oxidizing agent KMnO4 used for the oxidation reaction of rGO2. The phenolic functional groups in rGO were investigated by de-convolution of the singlet O 1 s peaks into three individual segments, designated as OX, OY and OZ at 532, 533.4 and 535.4 eV, respectively (Fig. 3b and d). Segments OX, OY and OZ were assigned to C = O (oxygen double bond to aromatic carbon), C–O (oxygen single bond to carbon) and C-OH (carbon single bond to the hydroxyl group), respectively20,23. These peaks chemically shifted to 531.5, 533.2 and 534.9 eV in the rGO2 sample, i.e., slightly smaller binding energies, indicating a larger electronic charge on the oxygen atoms. This behavior further describes higher oxidation of rGO2. The OY/OX + OZ and OY/OZ ratios were larger in rGO2 (6.3 and 16.33) compared to rGO1 (4.23 and 7.2), indicating more carboxyl and carbonyl groups in the rGO2 sample. This result suggests denser epoxy network at the basal plane and a larger content of carbonyl linked at the edges of the graphene sheets in rGO2 sample compared to rGO1, associated with the harsher oxidation reaction in rGO220,22.
In these samples, Raman spectra showed D and G bands at 1350 cm–1 and 1587 cm–1, respectively (Fig. 4). It is known that the D band arises due to A1g symmetry and originates from the zone boundary phonons. This is attributed either to various defects or to a breakdown of translational symmetry in the graphite lattice. However, the G band is first-order scattering, related to E2g symmetry and corresponds to the Brillouin zone of crystalline sp2 lattices in graphite24,25. The higher I(D)/I(G) ratio in the rGO2 sample indicates larger defect density (Fig. 4)25,26. Therefore, the Raman results indicate that the rGO2 contains a larger density of structural defects. The XPS results suggest that these defects are epoxy and carbonyl/hydroxyl functional groups at the basal plane and the edges of the graphene sheets, respectively. The larger defect is formed by unzipping of the carbon segments in the basal plane and developing epoxy network22. This network distorts the translational and periodic symmetry of graphite flakes.
FTIR spectroscopy further revealed differences in functional groups between both types of rGO (Fig. 5a). In rGO1 sample, the –CH2 absorption band was split into two sub-bands centered at 2855 cm–1 (symmetric) and 2923 cm–1 (asymmetric) stretching modes, assigned to alkyl moieties (as a result of the reduction of COOH to -CH3 segment)27,28. These bands are very weak in these samples, indicating small amount of functionalized hydrogen moieties with carbon network.
A stretching band at 3435 cm–1 was related to the C–OH group and it was stronger in rGO1 sample, indicating a larger content of hydroxyl groups20. However, the absorption band intensities of –C–O (alkoxy) and –C–O (epoxy) groups at 1050 cm–1 and 1220 cm–1, respectively, were weaker in rGO1 sample. This is expected when concentration of oxidizing substances such as KMnO4 is not sufficient to break the strong covalently bonded carbon symmetry at the basal plane. In this condition, most of the oxygen groups will functionalize the edge of the graphene planes without producing lattice distortions and defects at the basal planes. The peak at 1650 cm–1 was attributed to the bending of O–H or C = C stretching, indicating stability of the graphene structure27,28. This peak was stronger in both the rGO1 and rGO2 sample and this is in agreement with the XPS data, indicating structural integrity. The shift of this peak to lower wave numbers in rGO2 sample may indicate stronger hydrogen bond coordination between the graphene-oxide sheets. This might be possible when hydroxyl-hydroxyl segments at the edge of the graphene sheets interact through hydrogen bonding22. Moreover, hydrogen bonding and electrostatic interaction between epoxy-hydroxyl units at the basal plane can also explain the peak shift, as hydrogen bond formation between C = O and O−H groups decreases the electron density of C = O due to electronic charge transfer from C = O to O−H antibonding orbital, thus lowering its vibrational frequency28. The FTIR analysis clearly indicates that rGO1 and rGO2 spectra were dominated by hydroxyl and epoxy-hydroxyl groups, respectively. Therefore, the coupling of the graphene-oxide sheets in rGO1 was expected to be facilitated via hydroxyl-hydroxyl interactions, mostly at the edges of the graphene sheets, as schematically shown in Fig. 5b. However, in the rGO2 sample, coupling of graphene sheets is expected to be predominantly through epoxy-hydroxyl interaction forming hydrogen bonding between the basal plane and edges of the graphene sheets (Fig. 5c). This fact is supported by the appearance of a shoulder at lower 2θ in XRD. In this sample, the presence of hydroxyl functional units at the edge of graphene sheets may also provide hydrogen bonding between networks of graphene sheets.
The chemical and structural characterization therefore indicates that rGO1 is mostly made of graphene sheets functionalized by hydroxyl groups at their edges facilitating inter-plane interactions. rGO2 is characterized by a larger density of oxygen-related functional groups, with many of them being epoxides residing on the graphene basal planes, in addition to hydroxyl groups, due to the harsher oxidizing conditions used in the manufacture of rGO2. Therefore, stronger inter-plane interactions are suggested in rGO2.
Chemical characterization of PEG and rGO/PEG blends
The FTIR spectra of PEG200 and PEG600 showed a strong absorption band at 2870 cm–1, assigned to the –CH2 stretching vibration in alkyl chains (Fig. S1 in Supplementary Information). Peaks at 1353 cm–1 and 1498 cm–1 were ascribed to aliphatic C–H deformation29. The absorption band at 1062 cm−1 describes stretching vibration of the –C–O–C group attributed to the repeating oxyethylene (–OCH2CH2–) units of the PEG backbone. The band at 3410 cm−1 was ascribed to the stretching mode of C–OH in PEG200, which shifted to 3470 cm−1 and became weaker in PEG600 due to weak inter-molecular hydrogen bonding and smaller amount of hydroxyl units28,29,30. The increase in the ratio of –CH2/O–H stretching mode peak intensities in PEG600, indicate dispersive interactions between backbones of –CH2 units. However, in PEG200 intermolecular interactions are dominated by hydrogen bonding through hydroxyl-hydroxyl units. The wetting characteristics qualitatively describe the polarity of the molecules. This was studied by contact angle measurement, which showed a higher value (82°) for PEG600 than for PEG200 (65°) on steel substrates (Inset of Fig. S1). The enhanced wetting characteristic of PEG200 can be explained by the shorter chain length and the larger amount of hydroxyl end groups, which interact through hydrogen bonding with the polar metal-oxide surface containing hydroxides. Wetting properties also depends on the cohesive strength of molecules, which is stronger in PEG600 due to longer chain length and stronger dispersive forces, enhancing anti-wetting behavior.
The coupling of two different oxygen functionalized rGOs with two different types of PEGs, and the chemical interactions between these substances were investigated towards understanding the friction and wear mechanism. The preparation method of the samples for analyzing interaction between graphene oxide and PEG is provided below in the experimental methods section. This interaction was investigated by FTIR absorption spectroscopy and the results are shown in Fig. S2a. All FTIR absorption spectra showed a shift of the epoxy (C–O–C) vibrational mode to a higher frequency due to coordination of epoxy groups at the basal plane of graphene sheets with PEG molecules. In this case, the PEG molecules get intercalated in the basal plane gallery of epoxy-hydroxyl functionalized rGO2 sample (Fig. S2b). This is the appropriate reason for the appearance of shoulder peak in XRD at 2θ of 16.5° in rGO2 sample where interlayer spacing increased to 0.53 nm (Fig. 1). The similar behavior is shown by Wang et al.27. Most importantly, in these samples, the –CH2 bands at 2870 cm–1 and 2923 cm–1 becomes significantly stronger (Fig. S2) compared to neat rGO1 and rGO2 (Fig. 5). This clearly indicates coordination between alkyl moieties of PEG with graphene oxide samples (Fig. S2). The C = C and C–OH vibrational peak intensities were stronger and shifted to 1642 cm–1 and 3415 cm–1, respectively, when the rGO1 sample was functionalized with PEG200 and PEG600 (Fig. S2a spectra ai&bi). The absorption peak of C–OH was stronger in rGO1 functionalized by PEG200. In this sample, hydroxyl functionality dominated, and the coupling of graphene sheet and PEG molecules was expected through the hydroxyl and oxyethylene unit of graphene-oxide sheet and PEG27, respectively (Fig. S2c). Therefore, adsorption of PEG in the basal plane gallery is not expected in these samples, where epoxy units are not present on the graphene planes22. The interaction of PEG molecules with the oxygen functional group in the rGO2 sample showed a weak absorption band of the hydroxyl unit, but the absorption band of the epoxy group was stronger (Fig. S2a spectra ci&di), as expected from hydrogen bonding between the epoxy unit of rGO2 and the hydroxyl moieties of the PEG molecules. This relation is schematically drawn in Fig. S2b. Reduction of the hydroxyl peak intensity in PEG600 blended with rGO2 is characteristic of PEG600. The peak at 1721 cm–1 was ascribed to the C = O stretching vibration mode in the carboxylic functional group (–COOH), indicating possible hydrogen bonding between PEG and graphene oxide27,31,32. This peak was stronger in the rGO2 sample blended with PEG200 and PEG600 due to large amount of carbonyl and carboxyl complexes, in agreement with the XPS analysis (Fig. 3).
The Raman spectra of the blended samples showed increased I(D)/I(G) ratio (Fig. S3) compared to pure rGO1 and rGO2 samples (Fig. 4). This clearly describes enhancement of structural defects, such as planer defects, staking faults, edges, vacancies, and bond distortions24,25,33 following blending with PEG. This ratio is higher in rGO2 blended additives and this could be explained by inherent high defect density in this sample (Fig. 4). Furthermore, it is important to notice that the I(D)/I(G) ratio is higher in PEG200 blended rGO1 and rGO2 samples than in PEG600 blends. The increase in defect density is related to effective coupling between rGO and PEG200 molecules. This could be related to the larger number of hydroxyl and oxyethylene units in PEG200, as indicated by FTIR analysis, due to their coupling with hydroxyl functional groups in rGO. The coupling of PEG600 with rGO might have been weaker also due to larger molecular weight, which makes inter-plane intercalation more difficult.
We conclude that the analysis indicates weaker interactions of PEG600 with both rGO types compared to PEG200 due to the smaller amount of hydroxyl content and larger inter-chain dispersive interactions in PEG600. For similar reasons, PEG200 shows better wetting of steel surface due to stronger interaction with polar groups on the steel surface. When blended with rGO1, PEG molecules interact only with the graphene plane edges via hydrogen bonding with the hydroxyl groups there. However, when blended with rGO2, PEG molecules intercalation between the graphene planes was indicated, mediated by the on-plane epoxide groups, in addition to hydrogen bonding with hydroxyl groups.
Tribological properties of neat PEGs
The results of load dependent friction behavior of neat PEG200 and PEG600 are presented in Fig. 6a, and schematic diagrams of their molecular clusters are shown in Fig. 6b and c. In-situ detailed friction data are presented in Fig. S4. These experiments served as controlled experiments and helped to select load points for comparison with rGO-blended PEGs. The friction coefficient of PEG600 was found to be lower than that of PEG200, and for both lubricants, this value decreased with increasing normal loads, which is explained by the shear-thinning of lubricant layer and a decrease in the intermolecular friction in the confined volume34. An increase in the friction coefficient at 15 N loads in PEG200 was observed. This may have been caused by a critical reduction of the lubricant film thickness in the contact, where critical boundary lubrication regime gives rise to shear resistance between the molecular segments of PEG. In this condition, the role of the lubricant becomes ineffective, while friction between solid metal surfaces dominates35,36. However, the viscosity of PEG600 is higher than that of PEG200 due to larger intermolecular dispersive forces (see Fig. S1 in Supplementary Information and related discussion), causing resistance to boundary-lubrication condition, hence no increase in friction coefficient was noted at higher loads.
The friction coefficient of PEG600 was found to be smaller than that of PEG200 throughout the entire measured load range. Intermolecular shear resistance in liquid generally increases with the viscosity, as expected for PEG600 (see above)26,28. An increase in the shear modulus of high molecular weight PEG was confirmed by Ping Wang et al.37. For larger PEG molecules, polymer coils resist the shear stress, which appreciably contributes to the shear modulus. The PEG600 should show higher friction coefficient due to high viscosity, increased internal friction and high shear modulus, however the results showed a different behavior. The reasons for the lower friction coefficients of PEG600 might include increase of inter-molecular repulsive forces in stressed conditions due to a decrease in the inter-molecular distance of methylene units. The reduced friction coefficient might also be related to reduced shear due to directional degree of freedom of longer methylene units in PEG600 and the smaller density of cross-linking hydrogen bonded functional groups12,38,39,40,41,42, as schematically shown in Fig. 6c. The hydroxyl groups of the PEG also interact through hydrogen bonding with hydroxides present at the steel surface40. This is the reason for the decrease in contact angle of PEG200, indicating better affinity to the steel surface, as discussed above with respect to FTIR and contact angle analysis. This could also explain the higher friction coefficients of PEG200.
Friction properties of PEG/rGO blends
The friction results of the rGO1 and rGO2 samples as a function of the additive concentration in PEG200 and PEG600 at 1 N and 5 N are shown in Figs 7 and 8. Detailed in-situ friction data is given in Figs S5–S8.
The friction coefficient of blends of rGO1 and rGO2 in PEG600 were lower than those of blends with PEG200, in accordance with the neat PEG properties discussed above. rGO1 blended in PEG200 and PEG600 showed higher values of the friction coefficient than rGO2 under both loading conditions (Figs 7 and 8), with values comparable to those of neat PEGs at these loads (Fig. 6a). However, rGO2/PEG blended samples showed significantly smaller friction coefficients. These observations could be directly related to the types of functional groups available in rGO samples, and to the chemical properties of the two different PEGs, both affecting the coupling of functionalized rGO sheets with PEGs. Hydroxyl and epoxy-hydroxyl groups were found to be dominant in the rGO1 and rGO2 samples, respectively (see above). The principal interaction mechanisms in the rGO1 sample include electrostatic attraction between the oxygen atom in one layer and the carbon atom of the C–O moieties in an adjacent layer17, and hydroxyl-hydroxyl interactions through electrostatic forces. The primary interaction mechanism observed in the rGO2 sample was the epoxy-hydroxyl interaction via hydrogen bonding (Fig. 5). The binding energy was stronger in the latter type of interaction17. Wang et al.17 have shown that epoxy-epoxy and hydroxyl-hydroxyl interactions between functionalized graphene sheets induced a smaller critical sliding force than hydroxyl-epoxy interactions. In this regard, the friction coefficients should have been lower in the hydroxyl-dominated graphene sample, i.e., rGO1, but the results of the rGO/PEG blends showed the opposite. However, in rGO1/PEG blends, the PEG was coupled through the hydroxyls at the graphene edges and the oxygen of the oxyethylene units in PEG. This kind of coupling did not contribute to decreasing in shear resistance because the PEG molecule did not intercalate between the graphene planes18. The friction mechanism in hydroxyl-dominated graphene oxide (rGO1) sample is schematically shown in Fig. 9a. Here, edge functionalized graphene-oxide sheets interact with PEG and may lubricate the steel-steel contacting interfaces. In contrast, rGO2 was predominantly functionalized by the epoxy groups, allowing coupling of hydroxyl units of the PEG with oxygen of the epoxy units at the basal plane in rGO2 sample. Inter-layer shear of the graphene sheets was enabled by the intercalated PEG molecules, explaining reduction of the shear resistance. This is schematically presented in Fig. 9b. In both rGO1 and rGO2 blends the friction coefficients were almost concentration independent (Figs 7 and 8). Therefore, an extremely small amount of rGO2, e.g. 0.02 mg/mL, is sufficient to effectively lubricate the steel-steel sliding contact. The contact condition of linear reciprocating sliding mode is shown in Fig. 9c.
Here, PEG blended rGO sheets formed a boundary tribofilm in the tribo- contact and these are represented in Fig. 9a and b. Under the continuous sliding motion, these sheets get adsorbed at the surface of metallic tribo- contact, forming permanent and sustainable boundary tribofilm (Fig. 9c). The evidence of tribolayer is characterized in the later section.
Wear properties of PEG/rGO blends
Wear track analysis showed significantly smaller wear track width in PEG200 compared to PEG600 due to the strong wetting of PEG200 on steel surface (see above) that forms a high strength boundary film, minimizing the metal-to-metal contact which enhanced the antiwear properties (Fig. S9a). Selective wear tracks were subjected to 2-dimensional quantitative analysis and wear rate calculations. For this purpose, wear tracks formed at 1 N and 5 N loads with blends with 0.1 mg. mL–1 rGO1 and rGO2 additives with PEG200 and PEG600 were selected. The wear tracks and ball scars impression are presented in Fig. S10a–h. Highly effective antiwear behavior was observed in both rGO1 and rGO2 blended PEG200 lubricant at 1 N load (Fig. 10a), where the smallest damage of sliding bodies was observed in optical images (Fig. S10a and b). However, the wear loss was higher in rGO1 and rGO2 blended PEG600 at similar tribo-test conditions (Fig. 10c). Furthermore, at higher loads (5 N), both sets of samples lost the antiwear properties (Fig. 10b and d), similar to the neat PEG behavior (Fig. S9a). Therefore, it is clear that antiwear property of PEG200 is intrinsic characteristic of the PEG molecules. No clear relationships of concentration-dependent wear resistance were observed in both the additives blended PEGs, but the wear loss increased at high loads (Fig. S9c and e). This is clearly observed in 2-dimensional profiles of the wear tracks (Fig. 10b and d). This might be explained by smaller thickness of the lubricant layer in the sliding interfaces due to higher contact stress. In this condition, boundary lubrication operates where direct metal to metal contact dominates.
Moreover, results showed smaller wear track dimensions in the case of rGO1-compared to rGO2- blended in both PEG200 and PEG600. This is associated with intrinsic characteristics of hydroxyl terminated rGO sample which effectively protect against wear. It was noticed that antiwear performance was extremely good in the rGO1 sample at 1 N load (Fig. 10a), but the friction coefficient was very high under similar tribo-condition (Figs 7 and 8). In contrast, the wear track dimension was roughly doubled in the rGO2 sample at similar tribology conditions. In all the tribo-test conditions, the rGO1 sample was superior for wear resistance (Fig. 10). Calculation of wear rate also clearly showed high wear resistance of rGO1 sample (Fig. 10e). This calculation was carried out using the simple relation, k = W/F.s, where k, W, F and s are the wear rate, wear volume, normal force and sliding distance, respectively. Improved wear resistance properties of the blends could result from two factors: (a) hydrophilic properties of PEG200, which inherently protects the surface against wear forming boundary film. This is independent of the chemical properties of rGO1 and rGO2, and (b) rGO1 is hydroxyl functionalized and the compressive strength of such a functionalized structure is higher than that of rGO2. This is because rGO1 functionalization creates few defects on the plane of the graphene sheets as compared to epoxy functionalization of rGO222,43, as hydroxyl groups mostly occupy the edges of the graphene sheets22, in agreement with Raman and FTIR analysis (Figs 4 and 5). Tribology results of neat rGO1 and rGO2 sample without PEG are presented in Fig. S11 and it showed extremely low frictional coefficient in rGO1 sample, as expected. It can therefore be concluded that PEG200 and rGO1 blends provide the best anti-wear properties due to favorable combination of the constituents’ properties.
Spectroscopic analysis of wear tracks
Decrease in friction coefficient and high wear resistance properties could be traditionally explained by deposition of the graphene sheets at the tribo-contact region1,10. The presence of these sheets in the contact interfaces are directly related to dispersion stability and chemical interaction of the functionalized graphene sheets with the lubricant oil. The interaction aspect of functionalized graphene sheets with the lubricant is shown in Fig. S2 and the friction mechanisms are schematically drawn in Fig. 9. Hence, a chemical analysis of the wear track was carried out by Raman and XPS to provide evidence of tribolayer. Micro-Raman spectra of the wear track mainly showed a signature of metal-oxide and carbon peaks (Fig. S12). A very weak and diffused carbon signal in the wear track indicated the amorphous and elemental nature of carbon, which is inherently present (0.03%) in the steel substrate (316 LN). This was confirmed by the Raman spectra obtained from the steel surface (Fig. S12, spot (a)) of the same material, which showed a similar type of Raman shift to that of the wear track (Fig. S12, spots (b-d)). Therefore, evidence of carbon deposition from the rGO blended lubricant on the surface was not provided by Raman analysis. It is important to note that Raman spectroscopy is not a surface sensitive technique and chemical signals are mostly obtained from the subsurface region. However, XPS spectra at different locations of the same wear track showed prominent features of carbon and oxygen species (Fig. 11b). In these spectra, three photoelectron emission bands, i.e., segments C–C/C–H (284.4–284.8 eV), C–O/C–OH (285.6–286 eV) and C = O (287.5–289 eV)20,23 were designated as CX, CY and CZ, respectively. The chemical shifts at the wear track surface showed similar photoelectron emission characteristics to those shown of rGO2 sample (Fig. 3). The intensity of the C–O/C–OH peak in the wear track was enhanced compared to the virgin rGO sample. This might have been caused by the tribo-induced structural disordering of the graphene, and/or to oxidation of the graphene sheets during the tribology test. This evidence supports the deposition of chemisorbed rGO sheets on the surface of the wear track. The chemical shifts designated by the CX, CY and CZ segments were also present at the virgin steel surface, but their intensity was significantly weaker under similar XPS experimental conditions (Fig. 11a). The presence of oxygen species deduced from the O 1 s spectra in the virgin steel surface was also compared with that at various locations on the wear track (Fig. 11b).
Segments OX, OY and OZ in the wear track are associated with the interaction of carbon with oxygen species in various chemical configurations and oxidation states. The shapes and chemical shifts of these photoelectron emission peaks are quite similar to the as-prepared rGO samples (Fig. 3). However, the relative intensity of the OZ segment was increased in the wear track compared to the steel surface, indicating the presence of rGO moieties. From the spectroscopic results, it is concluded that the deposition of oxidized carbon species in the wear track has occurred, though a contribution of carbon inherently present in the steel surface cannot be ruled out. These observations confirm that graphene/graphene-oxide moieties are adsorbed on the surface of the wear track and participate in the lubrication process.
Two different reduced graphene oxide (rGO) derivatives were prepared for tribological investigation and blended with two different molecular weights of polyethylene glycol (PEG). Chemical and structural characterization indicated that rGO1 is mostly made of graphene sheets functionalized by hydroxyl groups at their edges facilitating inter-plane interactions. rGO2 is characterized by a larger density of oxygen-related functional groups, with many of them being epoxides residing on the graphene basal planes, in addition to hydroxyl groups, due to the harsher oxidizing conditions used in the synthesis of rGO2. Weaker interactions were found for PEG600 with both rGO types compared to PEG200 due to the smaller hydroxyl content and larger inter-chain dispersive interactions in PEG600. When blended with rGO1, PEG molecules interact only with the graphene plane edges via hydrogen bonding with the hydroxyl groups there. However, when blended with rGO2, PEG molecules intercalation between the graphene planes was indicated, mediated by the on-plane epoxide groups, in addition to hydrogen bonding with hydroxyl groups.
The friction and wear properties of PEG with two different molecular weights, namely PEG200 and PEG600, were compared in steel-steel contact interfaces. The higher molecular weight of PEG600 showed a lower friction coefficient, explained by the longer methylene-chain unit and enhanced anti-wetting properties, indicating effective boundary film lubrication. PEG200 showed higher values of the friction coefficient due to a strong wetting of the sliding interfaces. These results were compared with the tribological properties of PEG blends with the two different rGO additives functionalized by hydroxyl and epoxy-hydroxyl groups. Epoxy-hydroxyl functionalized rGO2-containing blends showed significantly lower friction coefficients compared to hydroxyl-terminated rGO1 additives blended in both types of PEGs. This was explained by intercalation of PEG molecules between the basal planes of the graphene sheets through epoxy-hydroxyl interactions between rGO2 and PEG. This decreased shear resistance of the sliding sheets and further reduced the frictional energy at the steel-steel interfaces. An extremely small concentration of rGO2, e.g. 0.02 mg/mL, was found to be sufficient to effectively lubricate the steel-steel sliding contact.
The mechanism of friction is well explained by adsorption of graphene/graphene-oxide sheets in the tribo-contact region which act as low shear strength boundary film, as demonstrated by XPS analysis performed in the various locations of the wear track. The antiwear properties were superior in hydroxyl-terminated rGO1. This was explained by a smaller defect density induced by the functional groups in the planes of the graphene sheets, which preserved the mechanical integrity of the graphene clusters to sustain the load bearing capacity of graphene-oxide boundary film. This kind of lubricant additives is easy to prepare and may be suitable for various potential applications. We summarize that rGO1 reduces wear but increases friction, while rGO2 reduces friction but does not effectively reduce wear.
Synthesis of hydroxyl-terminated rGO (rGO1)
The sample was prepared by Hummer’s method44,45. Graphite flakes (10 g) and NaNO3 (10 g) were mixed in 500 mL of H2SO4 (98%) at 5 °C with continuous stirring for 2 h, and KMnO4 (30 g) was gradually added to the suspension at a controlled reaction temperature lower than 15 °C. The ice bath was then removed, and the mixture was stirred at 35 °C until it became pasty brownish; stirring continued for two days, after which the mixture was diluted with a slow addition of 300 ml of water. The reaction temperature was rapidly increased to 98 °C, and the color changed to dark brown. This solution was further diluted by adding an additional 400 ml of water and stirring continuously. The solution was finally treated with 150 ml of H2O2 to terminate the reaction, indicated by the appearance of a yellow color. For purification, the mixture was washed by rinsing and centrifugation with 10% HCl and then with deionized water (DI) several times. After filtration and drying under a vacuum at room temperature, the GO1 was obtained as powder. Reduction was performed to reduce the functional group density, towards decreasing the inter-plane spacing and the flake dimensions and improving the friction properties. Reduction was done via treating 100 mg of GO1 in 30 mL of water with 3 mL of hydrazine and refluxing at 95 °C for 24 h, followed by filtering, washing and drying at 60 °C under vacuum to obtain the rGO1 powder.
Synthesis of epoxy-hydroxyl-terminated rGO (rGO2)
Graphite flakes (10 g) and NaNO3 (10 g) were mixed in 600 mL of H2SO4 (98%) at 5 °C with continuous stirring for 6 h, and KMnO4 (60 g) was gradually added to the suspension while maintaining the temperature at 15 °C. The mixture was diluted with a slow addition of 400 mL of water and with stirring maintained for 2 h. The ice bath was then removed, and the mixture was stirred at 35 °C for 2 h and then refluxed at 98 °C for 30 min. The solution was finally treated with 200 ml of H2O2 and the color changed to bright yellow. The resulting mixture was washed by centrifugation with 10% HCl and then with DI water several times until it became gel-like. After centrifugation, the gel was vacuum dried at 80 °C for 8 h to obtain the GO2 powder. Reduction was performed similarly to rGO1.
PEG and rGO-PEG blends
Two different molecular weights of PEG200 and PEG600 (from Sigma Aldrich) were used as synthetic lubricating base oils for tribology evaluation of the rGO additives. The average number of oxyethylene units in PEG200 is approximately 4 and its viscosity is 8.5 cSt. Viscosity of PEG600 is 18 cSt, and the average number of oxyethylene units is 13. The higher viscosity is caused by stronger intermolecular dispersive forces. Both rGO samples were dispersed and ultrasonicated for 3 h with a concentration of 1 mg/mL in PEG200 and PEG600. The samples were centrifuged, thoroughly washed in ethanol and DI water, and heat treated at 130 °C for 8 h to remove physisorbed PEG, ethanol and water molecules. Chemical analysis was applied to the dry powder samples of PEG200 and PEG600 functionalized by rGO1 and rGO2.
The surface topography of the rGO samples were analyzed by atomic force microscopy (AFM, Keysight 5500). For AFM analysis, the rGO samples were ultrasonicated in ethanol for 2 h, resulting in partial exfoliation. The flakes were deposited on silicon substrates that were kept inside the ethanol bath during ultrasonoication. Elimination of the oxygen functionalities from the rGO was the main reason for exfoliation. The microstructure and crystallography were further investigated by high resolution transmission electron microscopy (HR-TEM) and XRD pattern was obtained using a PAN-alyticalX’pert Pro dual goniometer consisting of a CuKα radiation source (λ = 0.15418 nm). The chemical composition was investigated by XPS (ULVAC-Phi ESCA1800), using a monochromatic MgKα source (400 W, 1253.6 eV) and by a micro-Raman spectrometer (Ranishaw) operating at a laser wavelength of 514.5 nm, which was also used for tribofilm analysis. An FTIR spectrometer (Bruker Optics), operating in transmission mode with a spectral resolution 4 cm−1, was used for the analysis of functional groups. Contact angle measurements of PEG200 and PEG600 on a steel surface were carried out using a contact angle meter (Holmarc, HO-IAD-CAM-01, India) equipped with a CCD camera. The volume of the droplet used for the contact angle measurement was approximately 1 μL.
Before the tribology test, the rGO was thoroughly dispersed in PEG by ultrasonication, and its dispersion stability was monitored. The tribological properties of the rGO dispersed in PEG were studied by measuring friction and wear at various loads, and rGO concentrations were measured using a ball-on-disc standard tribometer (CSM Instrument, Switzerland), operating in a linear reciprocating mode. A 100Cr6 spherical steel ball with a diameter of 6 mm was used to slide against a lubricated steel (316 LN) disc at a sliding speed of 4 cm/s. The surface roughness values of the ball and disc were approximately 32 and 17 nm, respectively. In each test, two drops of the ultrasonicated PEG blended with the rGO lubricant were used to thoroughly lubricate the sliding interfaces. A more detailed tribological experimental procedure is described elsewhere3,10. Two dimensional wear track profile were measured by a Dektak 6 M–stylus profiler in contact mode, at fixed 5 mg contact load and 10 μm/s scanning speed. In this method, the tip of the diamond stylus was scanned across the wear track generating 2D wear profile. All the tribological experiments and wear measurements were generally conducted four to five times and the error bars was represented with data. The reproducibility of the test was excellent and the value for error deviation was marginal. The stylus is mechanically coupled to the core of an LVDT sensor. Wear track image was obtained by optical microscope for damage and wear width analysis. Before the XPS analysis, the wear track was ultrasonicated in deionized water and dried at 110 °C to remove physisorbed contaminating particles.
How to cite this article: Gupta, B. et al. Role of oxygen functional groups in reduced graphene oxide for lubrication. Sci. Rep. 7, 45030; doi: 10.1038/srep45030 (2017).
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Mungse, H. P. et al. Synthesis, dispersion and lubrication potential of basal plane functionalized alkylated graphene nanosheets. RSC Adv. 5, 25565–25571 (2015).
Sarno, M. et al. Oil lubricant tribological behaviour improvement through dispersion of few layer graphene oxide. J. Nanosci. Nanotechnol. 14, 4960–4968 (2014).
Mungse, H. P. et al. Chemically functionalized reduced graphene oxide as a novel material for reduction of friction and wear. J. Phys. Chem. C. 118, 14394–14402 (2014).
Jinshan, L. et al. Modification of graphene platelets and their tribological properties as a lubricant additive. Tribol. Lett. 41, 209–215 (2011).
Diana, B. et al. Graphene: a new emerging lubricant. Mater. Today. 17, 31–42 (2014).
Suk, J. W. et al. Mechanical properties of monolayer graphene oxide. ACS Nano 4, 6557–6564 (2010).
Bradley, D. Is graphene safe? Mater. Today. 15, 230 (2012).
Dou, X. et al. Self-dispersed crumpled graphene balls in oil for friction and wear reduction. PANS 113, 1528–1533 (2016).
Diana, B. et al. Extraordinary macro scale wear resistance of one atom thick graphene layer. Adv. Funct. Mater. 24, 6640–6646 (2014).
Gupta, B. et al. Chemically grafted graphite nanosheets dispersed in Poly(ethylene-glycol) by γ-radiolysis for enhanced lubrication. RSC Adv. 5, 53766–53775 (2015).
Gupta, B. et al. Energy efficient reduced graphene oxide additives: mechanism of effective lubrication and antiwear properties. Sci. Rep. 6, 18372–18381 (2016).
Xiao, X. et al. Chain length dependence of the frictional properties of alkylsilane molecules self-assembled on mica studied by atomic force microscopy. Langmuir. 12, 235–237 (1996).
Jahanmir, S. Chain length effects in boundary lubrication. Wear 102, 331–349 (1985).
Dai, J. et al. Study on the surface energies and dispersibility of graphene oxide and its derivatives. J. Mater. Sci. 50, 3895–3907 (2015).
Park, S. et al. Colloidal suspensions of highly reduced graphene oxide in a wide variety of organic solvents. Nano Lett. 9, 1593–1597 (2009).
Konios, D. et al. Dispersion behaviour of graphene oxide and reduced graphene oxide. J. Colloid Interf. Sci. 430, 108–112 (2014).
Wang, L. F. et al. Atomic-scale friction in graphene oxide: an interfacial interaction perspective from first-principles calculations. Phys. Rev. B. 86, 125436–125436 (2012).
Kobayashi, M. et al. Tribological characteristics of polyethylene glycol (PEG) as a lubricant for wear resistance of ultra-high-molecular-weight polyethylene (UHMWPE) in artificial knee join. J. Mech. Beha. Biomed. Mater. 38, 33–38 (2014).
Mu, L. et al. Enriching hetero-elements in lignin as lubricating additives for bio-ionic liquids. ACS Sustainable Chem. Eng. 4, 1840–1849 (2016).
Pei, S. et al. The reduction of graphene oxide. Carbon 50, 3210–3228 (2012).
Prajwal, C. et al. Self assembly of functionalized graphene nanostructures by one step reduction of graphene oxide using aqueous extract of Artemisia vulgaris. Appl. Surf. Sci. 362, 221–229 (2016).
Dreyer, D. R. et al. The chemistry of graphene oxide. Chem. Soc. Rev. 39, 228–240 (2010).
Stobinski, L. et al. Graphene oxide and reduced graphene oxide studied by the XRD, TEM and electron spectroscopy methods. J. Electron Spec. Relat. Phenomena 195, 145–154 (2014).
Yang, D. et al. Chemical analysis of graphene oxide films after heat and chemical treatments by X-ray photoelectron and micro-Raman spectroscopy. Carbon 47, 145–152 (2009).
Ferrari, A. C. et al. Raman spectrum of graphene and graphene layers. Phys. Rev. Lett. 97, 187401–187404 (2007).
Kotakoski, J. et al. From point defects in graphene to two-dimensional amorphous carbon. Phys. Rev. Lett. 106, 105505–105508 (2011).
Wang, C. et al. Graphene oxide stabilized polyethylene glycol for heat storage. Phys. Chem. Chem. Phys. 14, 13233–13238 (2012).
Wang, H. et al. An effective non-covalent grafting approach to functionalizing individually dispersed reduced graphene oxide sheets with high grafting density, solubility and electrical conductivity. Nanoscale 7, 3548–3557 (2015).
Kumar, T. Fourier transform infrared spectrometric determination of polyethylene glycol in high-density polyethylene. Analyst 115, 1597–1599 (1990).
Gajendiran, M. et al. Gold nanoparticle conjugated PLGA–PEG–SA–PEG–PLGA multiblock copolymer nanoparticles: synthesis, characterization, in vivo release of rifampicin. J. Mater. Chem. B. 2, 418–427 (2014).
Joseph, J. & Jemmis, E. D. Red-, blue-, or no-shift in hydrogen bonds: aunified explanation. J. Am. Chem. Soc. 129, 4620−4632 (2007).
Gupta, B. et al. Effective noncovalent functionalization of Poly(ethylene glycol) to reduced graphene oxide nanosheets through γ-radiolysis for enhanced lubrication. J. Phys. Chem. C 120, 2139−2148 (2016).
Ferrari, A. C. & Basko, D. M. Raman spectroscopy as a versatile tool for studying the properties of graphene. Nature Nanotechnol. 8, 235–246 (2013).
Hsu, S. M. Molecular basis of lubrication. Tribol. Int. 37, 553–559 (2004).
Hsu, S. M. & Gates, S. R. Boundary lubricating films: formation and lubrication mechanism. Tribol. Int. 38, 305–312 (2005).
Bowden, F. P., Gregory, J. N. & Tabor, D. Lubrication of metal surfaces by fatty acids. Nature 156, 97–101 (1945).
Wang, P. et al. Molecular weight dependence of viscosity and shear modulus of Polyethylene glycol (PEG) solution boundary layers. J. Phys. Chem. C 113, 13793–13800 (2009).
Flory, P. J. Viscosities of linear polyesters. An exact relationship between viscosity and chain length. J. Am. Chem. Soc. 62, 1057–1070 (1940).
Saito, Y., Sasaki, N. & Komatsu, T. Molecular dynamics simulation for lubricant shear properties during heating. IEEE Trans. Magnetics 48, 209–2015 (2012).
Leszek, W. & Leszek, W. J. The influence of lubricant polarity on the boundary lubrication of sliding steel contacts. Wear 73, 87–93 (1981).
Cheng, H. & Yuanan, H. Influence of chain ordering on frictional properties of self-assembled monolayers (SAMs) in nano-lubrication. Adv. Coll. Interf. Sci. 171–172, 53–65 (2012).
Matthew, D. et al. Interfacial shear strength of multilayer graphene oxide films. ACS Nano. 10, 1939–1947 (2016).
Lizhao, L. et al. Mechanical properties of graphene oxides. Nanoscale. 4, 5910–5916 (2012).
Chen, J., Bowen, Y., Chun, Li. & Gaoquan, S. An improved hummers method for eco-friendly synthesis of graphene oxide. Carbon 64, 225–229 (2013).
Hummers Jr. W. S. & Offeman, R. E. Preparation of graphitic oxide. J. Am. Chem. Soc. 6, 1339–1339 (1958).
B.G. acknowledges DST, New Delhi, for Inspire Faculty Fellowship and the Blaustein Center for Scientific Cooperation for Blaustein Postdoctoral Fellowship. K.P would like to acknowledge the financial support from Japan Society for Promotion of Science (JSPS). The contribution of IITM, Chennai, India is acknowledged for TEM characterization. Ashok Bahuguna is greatly acknowledged for 2-dimensional profile of wear track measurement. N.K. dedicates this work to late Professor L.P. Yadav.
The authors declare no competing financial interests.
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Gupta, B., Kumar, N., Panda, K. et al. Role of oxygen functional groups in reduced graphene oxide for lubrication. Sci Rep 7, 45030 (2017). https://doi.org/10.1038/srep45030
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