(i)
Qj=i=1∑nFi∗δqiδri,j=1,2,...,m
(ii)
Qj=i=1∑nFi∗δq⋅jδVi,j=1,2,...,m (iii)
If
Ek=2mv2
Ek=Etotal−Ep=Etotal−mgh
We have
dtd(δq⋅iδL)−δqiδL=QinIn general, generalized forces can be considered as variations for the generalized coordinate in the term expression for virtual work.
Potential forces with all non-potential are taken into account. It is expressed through the Lagrange function L.
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