Gregg
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Homework Statement
## \gamma_1 ## and ##\gamma_2 ## are both real continuous solutions of ## \nabla^2 \gamma = \gamma ## in ## V## and ##\gamma_1=\gamma_2 ## on the boundary ##\partial V##. We are looking at the function ##g = \gamma_1 - \gamma_2 ##.
I have proved
##\nabla \cdot \left( g \nabla g) \right) = ||\nabla g||^2 + g\nabla^2 g## already. I used this to show that
##\int_V ||\nabla g||^2 dV + \int_{\partial V} g^2 dV = 0 ##
The question is: what does this say about the value of ##g=\gamma_1-\gamma_2 ## in ##V## and are the solutions unique for ##\nabla^2 \gamma = \gamma##?
Any help appreciated!
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