PhDorBust
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Given \frac{\partial^2 V}{\partial u \partial v} = 0, the solution is V_1(u) + V_2(v) for arbitrary V_1 , V_2.
I solve to get \frac{\partial V}{\partial u} = V_3(u) and then V = \int V_3(u) du + C Where V_3, C are arbitrary.
How could I transform my latter solution into the first solution? Don't V_1, V_2 have to have some properties such as differentiability? (I found this in a physics textbook)
I solve to get \frac{\partial V}{\partial u} = V_3(u) and then V = \int V_3(u) du + C Where V_3, C are arbitrary.
How could I transform my latter solution into the first solution? Don't V_1, V_2 have to have some properties such as differentiability? (I found this in a physics textbook)