A term of the type \( \frac{\partial T}{\partial q_k} \), where \( T \) and \( q_k \) are the kinetic energy and a generalized coordinate, respectively, if occurring in the equation of motion of a system is called a:
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In Lagrangian mechanics, generalized momentum is obtained by differentiating the kinetic energy with respect to the generalized velocity.
Generalized momentum is defined as:
\[
p_k = \frac{\partial T}{\partial \dot{q_k}}
\]
If \( \frac{\partial T}{\partial q_k} \) appears in the equation of motion, it refers to the generalized momentum.