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Titlebook: Computational Contact Mechanics; Geometrically Exact Alexander Konyukhov,Karl Schweizerhof Book 2013 Springer-Verlag Berlin Heidelberg 201

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楼主: hydroxyapatite
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Summary of findings and implications,ves. The fundamental issues such as existence and uniqueness of the solution of the Closest Point Projection procedure are intensively studied. In due course the CPP procedure leads to a special curvilinear coordinate system in which later all contact kinematics and weak forms are formulated separat
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Jan Kantowsky,Axel Schulte,Michael Baurl values, to formulate the weak forms for all considered contact situations: Surface-To-Surface, Point-To-Curve, Curve-To-Curve etc. in corresponding curvilinear coordinate systems. In addition various formulations of the Nitsche approach are discussed.
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Jan Kantowsky,Axel Schulte,Michael Baur for contact forces and stresses. With regards to the introduced coordinate system and kinematics the contact tractions are naturally split into normal and tangential components. If for the normal components non-penetration conditions can be formulated then for tangential components the constitutive
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Hedgefonds und Distressed-Debt-Investorenull linearization of the corresponding weak forms representing the equilibrium conditions on the contact boundaries described in Chapter 5 for all contact cases. Linearization is obtained using the covariant derivatives in the corresponding local surface coordinate system, where derivatives of conta
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https://doi.org/10.1007/978-3-8349-8380-0Sections 6.2, 6.3 and 6.4. The model, first, is implemented for the full Newton method and then the Augmented Lagrangian method. The tangent matrices is then based on the linearization derived in Sect. 7.3.
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https://doi.org/10.1007/978-3-8349-8380-0ces (originally published in [98]). The necessity to apply a coupled contact interface model including anisotropy for both adhesion and friction is shown in the current chapter via a set of experiments for a rubber surface possessing a periodical waviness, and therefore, an obvious anisotropic struc
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