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Constrained Planar Multibody Systems

The more general case is the constrained, planar system. A constraint is a relation between a subset of the coordinates, which must hold for every possible system configuration. A typical constraint is a joint, which allows motions parallel to certain axes only or restricts certain rotations, e.g. a Kardan joint. More complicated joints are constraints which permit motions only along a prescribed curve or surface. Typical technical examples for this type of joints can be found in contact mechanics, see Sec. 5.5. [Pg.17]

The equations of motion in the constrained case have the form [Pg.18]

the equations of motion for a holonomically constrained system have the structure [Pg.18]

Example 1.3.2 We modify now the truck given in Example 1.3.1 by replacing the spring and damper at the rear end of the loading area by a joint, which allows the loading area to be tilted, cf. Fig. 1.5. The constraint says that the distance between chassis and loading area at the joint s rotation axis must be zero. We must therefore compute the relative vector ps2 between the points of attachment of the joint 52 [Pg.19]

Altogether the equations of motion of the constrained truck are given by [Pg.20]


See other pages where Constrained Planar Multibody Systems is mentioned: [Pg.17]    [Pg.17]   


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