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A mechanical system, with generalised coordinates q_{1} and q_{2}, has Lagrangian L(q_{1}, q_{2}, q_{1}prime, q_{2}prime). State Lagrange's equations for the system, and deduce that q _{1}prime \frac{ delta L }{ delta q_{1}prime } (q_{1}, q_{2}, q_{1}prime, q_{2}prime) + q _{2}prime \frac{ delta L }{ delta q_{2}prime } (q_{1}, q_{2}, q_{1}prime, q_{2}prime) - L(q_{1}, q_{2}, q_{1}prime, q_{2}prime) is constant during the motion.
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