Mechanics of Fretting FatigueSpringer Science & Business Media, 09.03.2013 - 246 Seiten Failures of many mechanical components in service result from fatigue. The cracks which grow may either originate from some pre-existing macroscopic defect, or, if the component is of high integrity but highly stressed, a region of localized stress concentration. In turn, such concentrators may be caused by some minute defect, such as a tiny inclusion, or inadvertent machining damage. Another source of surface damage which may exist between notionally 'bonded' components is associated with minute relative motion along the interface, brought about usually be cyclic tangential loading. Such fretting damage is quite insidious, and may lead to many kinds of problems such as wear, but it is its influence on the promotion of embryo cracks with which we are concerned here. When the presence of fretting is associated with decreased fatigue performance the effect is known as fretting fatigue. Fretting fatigue is a subject drawing equally on materials science and applied mechanics, but it is the intention in this book to concentrate attention entirely on the latter aspects, in a search for the quantification of the influence of fretting on both crack nucleation and propagation. There have been very few previous texts in this area, and the present volume seeks to cover five principal areas; (a) The modelling of contact problems including partial slip under tangentialloading, which produces the surface damage. (b) The modelling of short cracks by rigorous methods which deal effectively with steep stress gradients, kinking and closure. (c) The experimental simulation of fretting fatigue. |
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Seite 3
... contacting bodies occurs , limited only by the coefficient of interfacial friction , and stick regions . It is the finite elasticity or com- pliance of the bodies which permits them to slip past each other in one region whilst sticking ...
... contacting bodies occurs , limited only by the coefficient of interfacial friction , and stick regions . It is the finite elasticity or com- pliance of the bodies which permits them to slip past each other in one region whilst sticking ...
Seite 4
... contacting bodies , to enable the engineer explicitly to avoid the conditions where a crack may initiate . However , if conditions are so arduous that the initiation of cracks is unavoidable , the influence of the fretting contact on ...
... contacting bodies , to enable the engineer explicitly to avoid the conditions where a crack may initiate . However , if conditions are so arduous that the initiation of cracks is unavoidable , the influence of the fretting contact on ...
Seite 9
... contact be incorporated , but many other aspects need to be carefully studied , too . In the flanged joint , for example , what is the pre - load provided in the bolts ? Are the contacting bodies elastically similar ? How is the size of ...
... contact be incorporated , but many other aspects need to be carefully studied , too . In the flanged joint , for example , what is the pre - load provided in the bolts ? Are the contacting bodies elastically similar ? How is the size of ...
Seite 11
... contact , i.e. its extent is not fixed geometrically , but is dependent on the applied load . Further , the contacting bodies have a common tangent at the edge of the contact , and the slope of the deformed surfaces is continuous there ...
... contact , i.e. its extent is not fixed geometrically , but is dependent on the applied load . Further , the contacting bodies have a common tangent at the edge of the contact , and the slope of the deformed surfaces is continuous there ...
Seite 12
... contacting bodies ( R in this instance ) . Figure 2.2 ( d ) shows another incomplete contact , formed by pressing a cylinder radially into a hole of only slightly larger diameter . Under these conditions the arc of contact is a ...
... contacting bodies ( R in this instance ) . Figure 2.2 ( d ) shows another incomplete contact , formed by pressing a cylinder radially into a hole of only slightly larger diameter . Under these conditions the arc of contact is a ...
Inhalt
5 | |
Contact of spheres the Hertz problem | 31 |
149 | 37 |
Contacts under Partial Slip | 41 |
Advanced Contact Mechanics | 65 |
9 | 101 |
26 | 108 |
41 | 115 |
60 | 149 |
1 | 169 |
Analysis of crack propagation | 175 |
Analysis of crack initiation | 199 |
Conclusions | 215 |
78 | 226 |
83 | 233 |
210 | 235 |
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Häufige Begriffe und Wortgruppen
applied arise asperity contact axi-symmetric behaviour bulk stress bulk tension Chapter coefficient of friction Comninou component compressive configuration constant contact patch contact problems contacting bodies crack faces crack initiation crack length crack propagation crack tip cyclic cylinders Dundurs effect elastically similar experimental Figure finite element finite element method fracture mechanics fretting fatigue fretting fatigue cracks fretting problems geometry given Green's functions half-plane hence Hertzian contact integral equation material Mech Mindlin mode normal load obtained occurs parameter partial slip plain fatigue plane plane strain plasticity possible predict region relative displacement relative slip residual stress shear force shear stress shear traction distribution shear tractions shown in fig singular sliding slip amplitude slip zones solution specimen spheres stick zone strain stress intensity factor surface displacements tangential displacement tangential force tangential loading technique tensile tests zero