How Can You Find the Inverse of the Exterior Derivative?

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SUMMARY

The discussion focuses on finding the inverse of the exterior derivative for a one-form represented as ##\omega = u dx + v dy##. The exterior derivative is given by ##d\omega = \left ( \frac{\partial v}{\partial x} - \frac{\partial u}{\partial y}\right )dxdy##. The equation to solve is ##d \alpha = \beta## for a ##p##-form ##\alpha## and a ##(p+1)##-form ##\beta##, which requires consistency with ##d^2 = 0##. While local solutions exist under these conditions, global solutions may not be attainable due to nontrivial topology of the manifold.

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If given an one-form like: ##\omega = u dx + v dy##, dω is ##d\omega = \left ( \frac{\partial v}{\partial x} - \frac{\partial u}{\partial y}\right )dxdy##. So, is possible to make the inverse path?

Given: ##d\omega = Kdxdy## , which is the expression for ω ?

##\omega = ? dx + ?dy##
 
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Generally what you want to do is solve

[tex]d \alpha = \beta[/tex]
for a ##p##-form ##\alpha## and a ##(p+1)##-form ##\beta##. In order for this equation to have a solution, it must be consistent with ##d^2 = 0##. So you must have

[tex]d^2 \alpha = d \beta = 0[/tex]
If that is true, then you can always find a local solution. However, you might not find a global solution if your manifold has nontrivial topology.
 

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