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Coulomb Friction Mathematical Background

In the preceding section we used a simple model containing Coulomb friction to demonstrate the problems when solving the equations of motion. We gave a refined model for this example. Now, we want to generalize this foregoing, i.e. we want to construct refined models for the general case of systems with jump discontinuities [Pg.213]

In the sequel we describe the problem of inconsistent switching and briefly introduce Filippov s approach. On this basis we construct an automatic treatment of this situation by a generalized three-valued switching logic. [Pg.214]

The problem of inconsistent switching is described for ordinary differential equa-tions of the form [Pg.214]

In the example given at the beginning of this section we have [Pg.214]

To overcome this difficulty, Filippov [Fil64] extended the definition of a solution for ordinary differential equations by allowing the right hand side to be any value of a set valued right hand side which consists of all convex combinations of / , /  [Pg.215]


See other pages where Coulomb Friction Mathematical Background is mentioned: [Pg.213]    [Pg.213]   


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