Resistance of a odd shaped conductor

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Homework Help Overview

The discussion revolves around calculating the resistance of an oddly shaped conductor, with participants exploring the implications of its irregular geometry on the application of relevant equations in electromagnetism.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Problem interpretation

Approaches and Questions Raised

  • Participants discuss starting points for the problem, including the use of Laplace's equation and the formulation of current density. Questions arise about how to express current density as a function of the conductor's geometry and how to derive voltage from it.

Discussion Status

Some participants have offered guidance on the relationship between resistance, voltage, and current, while others are exploring different methods to approach the problem. There is an ongoing exchange of ideas regarding the integration of circular cross-sections and the implications of variable radius on the calculations.

Contextual Notes

Participants note that the irregular shape of the conductor complicates the application of standard equations, and there are discussions about the assumptions related to current flow and resistivity. The relationship between the radius and height of the conductor is also under consideration.

jesuslovesu
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Homework Statement


http://img228.imageshack.us/img228/2536/physicsme1.th.png

Homework Equations



[tex]I = \int \int J . dS[/tex]
[tex]V = - \int E . dl[/tex]
[tex]V = IR[/tex]

The Attempt at a Solution


I'm not really sure how to get started on this problem, generally I would start with Laplace's equation but due to its irregular shape, I don't think that I can use that for this situation.
J is a function the length of the shape, but not sure how to formulate it into something useful
Does anyone know how I can get started on this?

[tex]I(z) = \int_0^h \int_0^{2\pi} \mathbf{J}(z) z d\phi dz[/tex]
 
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Hi jesuslovesu,

Here are a couple of points that may help.

The resistance of an object is R=V/I. Here you can assume that there is a constant current coming in one side of the resistor and leaving the other (and they must be the same-do you see why?) So if you can find the potential difference across the resistor that gives that current you'll be done.

The resistivity relates the current density and the electric field by

[tex] \vec J = \frac{\vec E}{\rho}[/tex]

You say you found an expression for [itex]\vec J[/itex]. How can you then find V?
 
Hey thanks for your reply, I've almost got it but I can't seem to quite get the last part.

So I say that [tex]J(z) = \frac{I}{\pi r^2}[/tex]
[tex]V = - \int_0^h \frac{I dz}{\sigma \pi r^2}[/tex]
[tex]\frac{I*h/(\sigma \pi r^2)}{I} = \frac{h}{\sigma \pi r^2}[/tex]
I've almost got it but I don't quite know what to do with the 'r', I am not positive if my integral is correct since J is a function of z
 
I would have approached it differently, but either way should be valid. I would have started with the equation for the resistance of a fixed-area element:

[tex]R_i = \frac{\rho L}{A}[/tex]

and integrated circular cross-sections of the conic section. Maybe give that approach a try...
 
r is a function of z. You have r(0) = a and r(h) = b
 

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