Show that use of the energy theorem (Problem 2) in the Lagrangian integral form of conservation of energy, d dt Vo 1 2 v · v + ε rhoo dVo = Vo (b · v + r) rhoo dVo + So (to · v − qo · no) dAo, leads to the pointwise (differential) form: rhoo ε˙ = To · ˙F + rhoo r − Div qo, where qo is the referential heat flux vector.

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step-by-step explanation:

idk the answer i want to say 10 but then it would be equal so try 9 but then yeah so yeah we love edgen

the answer is 0.000652422

but if you ment to ask what is 6131 divided by 4, it is 1532.75.

step-by-step explanation: