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Let \(V\) be a finite-dimensional vector space, let \(\omega\) be an alternating covariant \(k\)-tensor on \(V\), and let \(\eta\) be an alternating covariant \(l\)-tensor on \(V\). Then\[\omega\wedge\eta=\frac{\left(k+l\right)!}{k!l!}\text{Alt}\left(\omega\otimes\eta\right).\]What is the geometric interpretation of the wedge product?
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I am learning about wedge products to be able to integrate on manifolds. Is it then safe to assume that they are sort of infinitesimals?
@ganeshie8 @jim_thompson5910 @uri @thomaster These will be able to help you.
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