Ressistance when current-density is not constant

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SUMMARY

The discussion focuses on the relationship between resistance (R) and varying current density (J) in a wire with length (L) and a non-constant cross-sectional area (A(x)). The participant questions how to relate resistance to current density when the electric field (E) is not constant. It is established that despite the non-constant electric field, resistance can still be determined by calculating the electric field as a function of position (E(x)) and integrating it to find the potential drop, thereby allowing for the calculation of resistance.

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I am trying to figure out how it would effect the ressistance R of a wire with length L and variyng cross-sectional area A(x) if the current density was a fuction of the radius of the wire. That is J = J(r).

I'm having trouble with this when it seems like ressistance is the result of a derivation of ohm's law assuming constant E-field such that [tex]E = \frac{J}{\sigma} = \frac{V}{l}[/tex], but if E is not constant how can one then relate the ressitance to the current-density J?

A qualitative answer is good enough.
 
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But if E is not constant how can one then relate the resistance to the current-density J?
Resistance is by definition ΔV/i(and this is not Ohm's Law).Even though the electric field is not constant it is a law accurate for differential elements. So if you calculate E(x) function and integrate for the corresponding potential drop you can calculate resistance.
 

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