Abstract
The friction effects in the joints are assumed to be negligible. Figure 4.1 shows an arbitrary body with the total mass m. The body can be divided into n particles, the ith particle having mass, m i , and the total mass is \( m = \sum_{i=1}^{n} m_i \).
Keywords
Rigid Body Inertia Force Kinematic Chain Moment Equation Joint Force
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© Springer London 2009