Tensor field

Tensor field transformation laws

Let (𝑀,π’œ) be a 𝐢𝛼-manifold and 𝑋 ∈Tπ‘π‘ž(𝑀) be a tensor field. If π‘₯,π‘₯β€² :π‘ˆ,𝑉 →ℝ𝑛 are charts in π’œ, then in local coΓΆrdinates we have diff

π‘‹β€²πœ‡1β‹―πœ‡π‘πœˆ1β‹―πœˆπ‘ž(π‘₯β€²)=πœ•π‘₯β€²πœ‡1πœ•π‘₯𝛼1β‹―πœ•π‘₯β€²πœ‡π‘πœ•π‘₯π›Όπ‘πœ•π‘₯𝛽1πœ•π‘₯β€²πœˆ1β‹―πœ•π‘₯π›½π‘žπœ•π‘₯β€²πœˆπ‘žπ‘‹π›Ό1⋯𝛼𝑝𝛽1β‹―π›½π‘ž

Often physicists will take this as the definition of a tensor: β€œA tensor is an object whose components transform as a tensor.”


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