Question: Show that the function (L^{prime}) given in the preceding problem must obey Lagrange's equations if (L) does, directly from the principle of stationary action. Lagrange's

Show that the function $L^{\prime}$ given in the preceding problem must obey Lagrange's equations if $L$ does, directly from the principle of stationary action. Lagrange's equations do not have to be written down for this proof!

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