Results 111 to 120 of about 75,166 (160)
Some of the next articles are maybe not open access.
1985
This treatise is concerned with the stresses and deformation of solid bodies in contact with each other, along curved surfaces which touch initially at a point or along a line. Examples are a railway wheel and rail, or a pair of gear wheel teeth. Professor Johnson first reviews the development of the theory of contact stresses since the problem was ...
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This treatise is concerned with the stresses and deformation of solid bodies in contact with each other, along curved surfaces which touch initially at a point or along a line. Examples are a railway wheel and rail, or a pair of gear wheel teeth. Professor Johnson first reviews the development of the theory of contact stresses since the problem was ...
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Tribology International, 1998
Contact problems in the classical formulation are posed for topographically smooth surfaces; this ensures that the contact region will be continuous.
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Contact problems in the classical formulation are posed for topographically smooth surfaces; this ensures that the contact region will be continuous.
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Contact Mechanics in Multibody Systems
Multibody System Dynamics, 1998zbMATH Open Web Interface contents unavailable due to conflicting licenses.
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1994
Many real fretting problems involve the contact of components of great complexity, such as the flanged joints depicted in the pipework photograph, fig. 2.1. In cases such as this it is really quite impossible to consider modelling the contact by anything other than a numerical method, and the technique chosen will in many cases be the finite element ...
D. A. Hills, D. Nowell
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Many real fretting problems involve the contact of components of great complexity, such as the flanged joints depicted in the pipework photograph, fig. 2.1. In cases such as this it is really quite impossible to consider modelling the contact by anything other than a numerical method, and the technique chosen will in many cases be the finite element ...
D. A. Hills, D. Nowell
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2015
In this chapter, an asymptotic modeling methodology for tibio-femoral contact is developed, based on the asymptotic models of frictionless unilateral contact interaction between thin cartilage layers. In Sect. 7.1, the normal contact forces, which are needed for multibody dynamics simulations, are determined analytically based on the exact solution for
Ivan Argatov, Gennady Mishuris
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In this chapter, an asymptotic modeling methodology for tibio-femoral contact is developed, based on the asymptotic models of frictionless unilateral contact interaction between thin cartilage layers. In Sect. 7.1, the normal contact forces, which are needed for multibody dynamics simulations, are determined analytically based on the exact solution for
Ivan Argatov, Gennady Mishuris
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2016
In this chapter, we briefly discuss three hotly debated issues of the current research on adhesive foot pads, (1) the validity of the contact splitting theory and its implication for scaling laws, (2) the role of fluid secretions in hairy adhesive pads, and (3) the controversy about the subdivision of biological adhesive systems into ‘dry’ and ‘wet ...
Jonas O. Wolff, Stanislav N. Gorb
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In this chapter, we briefly discuss three hotly debated issues of the current research on adhesive foot pads, (1) the validity of the contact splitting theory and its implication for scaling laws, (2) the role of fluid secretions in hairy adhesive pads, and (3) the controversy about the subdivision of biological adhesive systems into ‘dry’ and ‘wet ...
Jonas O. Wolff, Stanislav N. Gorb
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Communications in Applied Numerical Methods, 1988
AbstractAn algorithm is given and proved for the solution of a strictly convex minimization problem with linear equality and inequality constraints, in a finite number of steps. It is used to solve frictionless and frictional problems in contact elastostatics, and it has the property that each step can be interpreted mechanically.
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AbstractAn algorithm is given and proved for the solution of a strictly convex minimization problem with linear equality and inequality constraints, in a finite number of steps. It is used to solve frictionless and frictional problems in contact elastostatics, and it has the property that each step can be interpreted mechanically.
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