A second-order tensor is a coordinate-independent linear map from vectors to vectors, where the input vector v produces an output vector T(v) = T_ij v_j, with one index contracting with the input and the other labeling the output; this distinguishes tensors from matrices, which are merely component representations after choosing a basis.
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Second-Order Tensor Explained Visually | Tensor as a Linear MapAdded:
A second-order tensor is not just a matrix. It is a linear map from vectors to vectors. Put in a vector v, and the tensor T returns a new vector T v.
The word linear is essential. If the input is alpha a plus beta b, the output is alpha T a plus beta T b. So the tensor respects vector addition and scalar multiplication.
The dyadic basis explains the two indices. The operator e i tensor e j tests the input along e j, then outputs along e i. Any second-order tensor can be built as T i j e i tensor e j.
Now act on a vector v equals v j e j. Using the dyadic rule, T v equals T i j v j e i. Therefore the component formula is T v sub i equals T i j v j. This is ordinary matrix multiplication written in tensor notation.
Final memory map. A vector has one index. A second-order tensor has two indices. One index contracts with the input, and one index labels the output. This is why stress maps a normal vector to a traction vector.
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