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Coulomb Friction Difficulties with Switching

Friction phenomena are often modeled by a law dated back to Coulomb. [Pg.210]

The friction force is assumed to be proportional to the normal force N on the surface between the two bodies in the contact point. The proportionality constant is the coefficient of friction /i which depends on the material properties of the surfaces and may depend on the velocity. [Pg.210]

In Coulomb s original model ji 0 has been assumed to be constant  [Pg.210]

The friction force is directed tangential to the friction surface and is opposite to the direction of motion of the body  [Pg.210]

Often this Coulomb friction is called dry friction. [Pg.211]

See other pages where Coulomb Friction Difficulties with Switching is mentioned: [Pg.210]    [Pg.211]    [Pg.213]    [Pg.215]    [Pg.217]    [Pg.219]    [Pg.221]    [Pg.223]    [Pg.210]    [Pg.211]    [Pg.213]    [Pg.215]    [Pg.217]    [Pg.219]    [Pg.221]    [Pg.223]   


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