Quick question about current density

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SUMMARY

The discussion centers on the calculation of current density (J) in a cylindrical cable using two different methods for determining area. The first method employs the formula for the surface area of the end of the cable, specifically using the equation π(r3² - r2²) for J2. The second method utilizes the integral ∫2πr dr to find the surface area along the inner cable, which is confirmed to represent the area of concentric rings. This distinction is crucial as the current density varies across these rings, necessitating the use of integration for accurate calculations.

PREREQUISITES
  • Understanding of current density (J) and its formula J=I/A
  • Familiarity with cylindrical coordinates and surface area calculations
  • Knowledge of integration techniques, particularly for circular areas
  • Basic concepts of electric current and its distribution in conductors
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  • Study the derivation of the formula for current density in cylindrical conductors
  • Learn about the application of integration in calculating areas of irregular shapes
  • Explore the concept of varying current density in multi-layered conductors
  • Investigate practical applications of current density in electrical engineering
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hahaha158
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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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