Maxwell stress tensor coordinate system

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The Maxwell Stress Tensor is coordinate-system dependent, and its expressions vary in different coordinate systems such as cylindrical and spherical coordinates. The general form provided by Griffiths applies to Cartesian coordinates, but adaptations are necessary for other systems. In cylindrical and spherical coordinates, the derivatives and components of the tensor must be adjusted accordingly. Understanding these adaptations is crucial for accurate calculations in various geometries. The discussion emphasizes the need for a new definition or transformation to correctly express the tensor in non-Cartesian systems.
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Hello,

I am trying to understand the Maxwell Stress Tensor. Specifically, I would like to know if it is coordinate-system dependent (and if so, what the expressions are for the stress tensor in cylindrical and spherical coordinates).

Griffiths gives the definition of the maxwell stress tensor in EQ8.19:
<br /> T_{ij} = \epsilon_0 (E_i E_j - \tfrac{1}{2} \delta_{ij} E^2) + \frac{1}{\mu_0} (B_i B_j - \tfrac{1}{2} \delta_{ij} B^2)<br /> <br />

where Griffiths says i and j can be x, y, z -- now can they also by r, z, phi or r, theta, phi? (or do we require a new definition for the stress tensor to handle cylindrical and spherical coordinates?)

Any comments would be really appreciated! Thanks!
Eric
 
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It would work in other orthogonal systems.
Derivatives get changed in the other systems.
 

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