User:John R. Brews/Sandbox: Difference between revisions

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Tensors can relate vectors of different dimensionality, as in the relation:
Tensors can relate vectors of different dimensionality, as in the relation:


<math> \begin{pmatrix}
:<math> \begin{pmatrix}
p_1\\
p_1\\
p_2\\
p_2\\
Line 16: Line 16:
\begin{pmatrix}
\begin{pmatrix}
T_{11} & T_{12} &T_{13}&T_{14}&T_{15}\\
T_{11} & T_{12} &T_{13}&T_{14}&T_{15}\\
T_{11} & T_{12} &T_{13}&T_{14}&T_{15}\\
T_{21} & T_{22} &T_{23}&T_{24}&T_{25}\\
T_{11} & T_{12} &T_{13}&T_{14}&T_{15}\\
T_{31} & T_{32} &T_{33}&T_{34}&T_{35}\\
T_{11} & T_{12} &T_{13}&T_{14}&T_{15}\\
T_{41} & T_{42} &T_{43}&T_{44}&T_{45}\\
T_{11} & T_{12} &T_{13}&T_{14}&T_{15}
T_{51} & T_{52} &T_{53}&T_{54}&T_{55}
\end{pmatrix}
\end{pmatrix}
\  
\  

Revision as of 19:13, 16 December 2010

Tensor

In physics a tensor in its simplest form is a proportionality factor between two vector quantities that may differ in both magnitude and direction. Mathematically this relationship is:

where v is a vector with components {vj} and w is another vector with components {wj} and the quantity Χ = {χij} is a tensor. This example is a second rank tensor. The idea is extended to third rank tensors that relate a vector to a second rank tensor, as when electric polarization is related to stress in a crystal, and to fourth rank tensors that relate two second rank tensors, and so on.

Tensors can relate vectors of different dimensionality, as in the relation: