Quick question about current density

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The discussion revolves around the confusion regarding the calculation of current density (J) using different surface area approaches. One method uses the surface area of the end of the cable, while the other employs an integral to find the area along the inner cable. The integral, ∫2πr dr, represents the area of concentric rings that account for varying current density across the cable. This distinction is crucial as the current density differs for each ring, necessitating the use of the integral. Understanding these methods clarifies how to accurately calculate current density in different scenarios.
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Homework Statement


Homework Equations



J=I/A

The Attempt at a Solution


I was just looking at the solution for this, and I was confused because they seemed to use different ways of finding the area. For finding J2, they took the surface area of the end of the cable, pi(r3^2-r2^2), but for finding J2, they took the area to be ∫2pir dr, which i think is the surface area along the inner cable. Why is one using the surface area of the end, and one using the surface area across the outside of an entire cable"?

thanks for any help
 
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hahaha158 said:
... but for finding J2, they took the area to be ∫2pir dr, which i think is the surface area along the inner cable.

∫2pir dr is actually the area of the end of the inner cable, ##\pi##R12, as you can see by carrying out the integral from 0 to R1. The integral is summing the areas of concentric rings that fill up the entire area. This is necessary since the current density is different for each ring.
 

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