Finding Solutions to $\frac{\partial^2 V}{\partial u \partial v} = 0$

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SUMMARY

The solution to the equation $\frac{\partial^2 V}{\partial u \partial v} = 0$ is definitively expressed as $V = V_1(u) + V_2(v)$, where $V_1$ and $V_2$ are arbitrary functions. The discussion further explores the derivation of $V$ through integration, leading to the expression $V = \int V_3(u) du + C$, where $V_3$ and $C$ are also arbitrary. The transformation from the latter solution to the former requires ensuring that $V_1$ and $V_2$ possess properties such as differentiability. The integration method can be adapted by switching the order of integration to equate the two results.

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Given [tex]\frac{\partial^2 V}{\partial u \partial v} = 0[/tex], the solution is [tex]V_1(u) + V_2(v)[/tex] for arbitrary [tex]V_1 , V_2[/tex].

I solve to get [tex]\frac{\partial V}{\partial u} = V_3(u)[/tex] and then [tex]V = \int V_3(u) du + C[/tex] 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)
 
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try the same method but integrate over the other variable first then equate the two results
 

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