By Kirsch U., Kocvara M., Zowe J.
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Additional resources for Accurate Reanalysis of Structures by A Preconditioned Conjugate Gradient Method
In addition to the heat equation for the body temperature, we discuss frictional heat generation and the heat exchange condition when the heat exchange coeﬃcient depends on the gap or the contact pressure. In Sect. 2 we describe the wear of the surfaces as a result of friction. 1), which is a rate condition for wear production. However, it does not allow for the diﬀusion or motion of the wear debris on the surface. When the wear particles or debris are harder than the surface material additional wear is caused.
4. (a) The function ke (η); (b) the graph ke ; η < 0 – contact; η > 0 – separation. pressure; when there is no contact ke = ksep (η) is a function of the gap. As contact is established or lost the value of the heat exchange coeﬃcient lies in the interval [ksep (0), kcon (0)]. The graph is depicted in Fig. 4(b). The graph reﬂects the experimental fact that it is very complicated to measure the heat exchange coeﬃcient when contact has just been established or lost ( [124, 125]). At the moment of initiation of contact certain surface asperities come in contact and deform during the contact period.
4a. In the second case ke was chosen as the graph, if η < 0 kcon (η) ke (η) = [ ksep (0), kcon (0)] if η = 0 . ksep (η) if η > 0 Here, when contact takes place ke = kcon (η) is a function of the contact 34 3 Additional Eﬀects Involved in Contact ke ke ✻ ✻ kcon ksep ✲ η ✲ η (a) (b) Fig. 4. (a) The function ke (η); (b) the graph ke ; η < 0 – contact; η > 0 – separation. pressure; when there is no contact ke = ksep (η) is a function of the gap. As contact is established or lost the value of the heat exchange coeﬃcient lies in the interval [ksep (0), kcon (0)].
Accurate Reanalysis of Structures by A Preconditioned Conjugate Gradient Method by Kirsch U., Kocvara M., Zowe J.