How to calculate the axial components for a helix?

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To calculate the axial components for a helix, the discussion highlights the use of the relation B = gradient crossed with A, but emphasizes the need for a clearer setup. The Poisson equation is suggested as an alternative method, with A(r) defined in terms of the current density J(r). Participants stress the importance of clearly defining variables, such as dτ, and choosing an appropriate coordinate system for the calculations. The conversation reflects a collaborative effort to clarify the mathematical approach needed for solving the problem. Effective setup and notation are crucial for accurate calculations in this context.
needphyshelpalways
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Homework Statement
Calculate the axial component of the vector potential A_vector at the center of a helix of 2N turns, of radius R , and of the length 2H, carrying a current I . (Need to calculate only the axial component of the vector potential, and only at the origin.)
Then show that the result (for the axial component of the vector potential at the origin) is the same as that for a single wire of length 2H along the side of the helix that carries a current I . Why is this so?
Relevant Equations
A(r) = (mu/4pi)integral{(J(r)/r}dtau
B = gradient crossed with A
I attempted to use the relation that B = gradient crossed with A; however, I'm strguggling with how to setup the question. I think that alternatively the problem can be solved using the Poisson equation that A(r) = (mu/4pi)integral{(J(r)/r}dtau; however, here to I am struggling with the setup.
 

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Hello needy, ##\qquad## :welcome: ##\qquad## !

needphyshelpalways said:
I attempted to use the relation that B = gradient crossed with A
Does that mean you already have A ? Probably not.

You only need the ##z##-component anyway. Can you write the integral a bit clearer ? In particular: what is ##{\mathrm d}\tau## ?
needphyshelpalways said:
I am struggling with the setup
Well, start with making a good choice of your coordinate system. Any ideas ? :rolleyes:
 

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