Surface Area Vector in Exterior Algebra 3D

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mikeeey
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Hello every one .
What is the Surface Area vector form in exterior algebra ,I mean by that the Surface Area vector as an exterior form in 3D , just like the volume form .THANKS
 
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yes its a 2-forms , but 2-form is a co-variant second order tensor , but here the surface area is a vector ,
this is why i want to know ,
in mechanics the stress distribution formula is [itex]F^i = \sigma^\ij dA_j[/itex]
where F is the force vector and (Sigma ) is the mechanical second order stree tensor and A is the Area vector
while in exterior algebra it's written like this [itex]F^i = T^i_jk dx^j\wedgedx^k[/itex]
where T is a third order tensor , when using calculus e.g. co-variant derivative , sigma with give 2 christoffel symbols while the T will give 3 christoffel symbols
 
[itex]F^i =\sigma^ij dA_j[/itex]
[itex]F^i= B^i_j_k dx^j \wedge dx^k[/itex]
 
The "surface area element" can be thought of as a "[3D-]vector" only in 3-D.
In the cross-product, the oriented parallelogram formed from the factors is more fundamental than the vector perpendicular to that parallelogram.
From a tensor algebra viewpoint, to get a vector from the oriented parallelogram,
one has to use the Hodge-dual (often symbolized by *), which involves the [itex]\epsilon_{ijk}[/itex] symbol.
 
you mean [itex]dA_i = \epsilon_ijk dx^j \wedge dx^k[/itex]
 
[itex]dA^i = \epsilon _{ijk} dx^j \wedge dx^k[/itex]
 
mikeeey said:
[itex]dA^i = \epsilon _{ijk} dx^j \wedge dx^k[/itex]

Yes, it's basically this, but you might have some normalization factors in there, I'm not quite sure.

EDIT: Oh, and in your formula the i has moved from lower index to upper index, so you have to raise the index in there somewhere. :)