Abstract
The equation system, described for kinematic pairs of Crank mechanism, consist of general constraint equations. For Crank mechanism, the position of the center of gravity for the components, and the directions of the main axis of inertia can be determined for the entire kinematic cycle. To determine the positions, we use a coordinate system fixed to the center of gravity of the mechanism. The coordinates of the center of gravity of the members of the mechanism are always constant in relation to the geometric system attached to the component. The vector contour created in this way, defined by position vectors, must always be closed.
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