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Tribological Properties of Structural Ceramics, edited by J. B. Wachtman, Jr. (Academic, San Diego, 1989); D. R. Clarke, Annu. Rev. Mater. Sci. 17, 254 (1987) and references therein; J. E. Marion, C. H. Hsueh, and A. G. Evans, J. Am. Ceram. Soc. 70, 708 (1987); D. Clarke, ibid. 70, 15 (1987).
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42
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85034283240
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note
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p is the pull-off force required to separate the two surfaces against the adhesion force between them (Fig. 1).
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43
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0000469962
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K. L. Johnson, K. Kendall, and A. D. Roberts, Proc. R. Soc. London, Ser. A 324, 301 (1971).
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Johnson, K.L.1
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Roberts, A.D.3
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44
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85034309208
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note
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2. The corresponding pressure is P=L/A, where the contact area A for this load is taken from Fig. 3 in Homola el al. (Ref. 53).
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45
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85034277838
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note
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Hu et al. (Ref. 40) have also reported values for the shear stress between mica surfaces sliding at different velocities across an OMCTS film confined to thickness n=3, at shear rates and normal pressures comparable to those in the present study. Their results, however [and also a more recent study from the same group (Ref. 41)], indicated viscous rather than solidlike response (no yield stress at zero frequency was observed), and so contrast with our data as well as with the data of Gee et al. (Ref. 20) and Yoshizawa and Israelachvili (Ref. 21). Possible reasons for the discrepancy have been considered in paper I (Ref. 34, preceding paper).
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52
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0020293551
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edited by J. M. Georges Elsevier, New York
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D. Tabor, in Microscopic Aspects of Adhesion and Lubrication, Tribology Series 7, edited by J. M. Georges (Elsevier, New York, 1982), pp. 651-682.
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Tabor, D.1
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55
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0003959123
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Clarendon Press, Oxford
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Similar ideas concerning the shear melting of bulk crystalline solids were discussed long ago [J. Frenkel, Kinetic Theory of Liquids (Clarendon Press, Oxford, 1946)].
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(1946)
Kinetic Theory of Liquids
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Frenkel, J.1
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56
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85034297583
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note
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A treatment somewhat in this spirit for shear of powder particles was presented by M. J. Adams (Ref. 7, p. 183) though in this model the friction between the powder particles themselves played a central role.
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58
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85005569706
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S. Granick, A. L. Demirel, L. L. Cai, and J. Peanasky, Isr. J. Chem. 35, 75 (1995).
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Granick, S.1
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Peanasky, J.4
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59
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0024749146
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A. M. Homola, J. N. Israelachvili, M. L. Gee, and P. M. McGuiggan, J. Tribology 111, 675 (1989).
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Homola, A.M.1
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McGuiggan, P.M.4
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62
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85034304515
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note
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c was subsequently suggested (Ref. 21) but is not considered here as Eq. (7) is thought to be more suited for liquids consisting of simple spherical molecules (Ref. 21).
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63
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85034283685
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note
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resonance of the shear-spring assembly (Ref. 34).
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64
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85034286284
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note
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-2/3, which was reported earlier (Ref. 40) for shear of some confined liquids, including thin films (n=3) of OMCTS. The reasons for the discrepancy have been discussed [see Ref. 39 and our preceding paper I (Ref. 34)].
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