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Recall from elementary school the generalized Stokes' theorem: for an orientable manifold $M$ and differential form $\omega$,
$$ \int_{\partial M} \omega = \int_M d\omega. $$
Recall from elementary school the generalized Stokes' theorem: for an orientable manifold $M$ and differential form $\omega$,
$$ \int_{\partial M} \omega = \int_M d\omega. $$