How to Perform a Cross Product on Polar Coordinates?

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Discussion Overview

The discussion centers on how to perform a cross product operation on vectors expressed in polar coordinates, particularly in the context of electromagnetic fields (E and H fields). Participants seek to understand the methodology without converting to rectangular coordinates.

Discussion Character

  • Exploratory, Technical explanation, Debate/contested

Main Points Raised

  • One participant requests a general method for performing a cross product on polar coordinates, specifically for E and H fields.
  • Another participant suggests that as long as vectors are expressed in terms of perpendicular unit vectors (like r-hat and theta-hat), the cross product can be performed in the usual way.
  • A participant presents a specific example of vectors in a matrix format, questioning whether the same cross product operation applies as in rectangular coordinates.
  • There is a clarification that the cross product operates in the tangent space rather than the coordinate space, emphasizing the use of an orthonormal basis at a point.
  • One participant expresses confusion about the representation of vectors and the need to cross-product fields at a general point.
  • Another participant provides an example of the cross product of unit vectors in polar coordinates, indicating that the operation remains consistent.

Areas of Agreement / Disagreement

Participants express varying levels of understanding regarding the application of the cross product in polar coordinates. Some agree on the use of unit vectors, while others raise questions about the representation and context of the vectors involved. The discussion remains unresolved with multiple viewpoints presented.

Contextual Notes

There are indications of confusion regarding the representation of vectors and the specific conditions under which the cross product is performed. The discussion highlights the need for clarity on the basis vectors used in polar coordinates.

tekness
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I would like to know how to perform a cross product on polar coordinates.

Thank You
 
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tekness said:
I would like to know how to perform a cross product on polar coordinates.

Thank You

Hi tekness! :smile:

Can you give us an example of two vectors you're trying to cross-product?
 
tiny-tim said:
Hi tekness! :smile:

Can you give us an example of two vectors you're trying to cross-product?


Hi tim,

I am just looking for a general way to perform the operation. I will perform a cross product between E and H fields that are in polar coordinates. I don't want to go through the hassle of converting back and forth :).

I hope this explains it, if not please let me know what else I can add.
 
tekness said:
I am just looking for a general way to perform the operation. I will perform a cross product between E and H fields that are in polar coordinates. I don't want to go through the hassle of converting back and forth :).

Well, so long as the vectors are expressed in terms of perpendicular unit vectors such as ihat and jhat or rhat and thetahat, you just cross-product them the usual way.

The only problem might be converting into unit vectors. :smile:
 
so for example.
I have |i j k|
|rcos() rsin() Z1|
|r2cos()2 r2sin()2 Z2|

the 2 is for a different value/angle.
So just perform the same cross product operation as rectangular coordinates would require?
 
tekness said:
so for example.
I have
Code:
|i                 j               k|
|rcos()         rsin()            Z1|
|r2cos()2     r2sin()2            Z2|

the 2 is for a different value/angle.
So just perform the same cross product operation as rectangular coordinates would require?

Hi tekness! :smile:

(have a theta: θ :smile:)

I'm a little confused … those look like vectors from the origin. :confused:

You will generally want to cross-product the fields at a general point.
 
I will try to verify exactly what I need and respond back. Looks like I need to rethink my question.
Thank you for your help! I will be back asap.
 
The confusion is that the cross product is an operation in the tangent space, not in the coordinate space. At a particular point, your field has components in the r-hat, phi-hat, and theta-hat directions. These three vectors constitute an orthonormal basis. So you simply take the cross product without any modification at all. For example,

\hat r \times \hat \theta = \hat \phi

and the rest are similar.
 

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