Electric Field at the End of a Line of Charge

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SUMMARY

The discussion focuses on calculating the electric field at a point on the x-axis due to a charged rod with a variable charge density described by λ=ax², where a=-20.2 μC/m³ and the rod length L=7.10 m. The user attempts to apply Coulomb's Law and integrate the electric field contributions from differential charge elements along the rod. The key challenge identified is correctly determining the distance from each differential charge element to the observation point, which is not constant across the length of the rod.

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  • Coulomb's Law for electric fields
  • Integral calculus for evaluating electric field contributions
  • Understanding of charge density and its implications
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Field at End of Line of Charge 2

A charged rod of length L=7.10 m lies centered on the x axis as shown. The rod has a charge density which varies according to λ=ax^2 where a=−20.2 μC/m^3 .

What is the x component of the electric field at a point on the x-axis a distance of D=3.70 m from the end of the rod?
media%2F71b%2F71ba0d9b-0e30-4c4b-8021-8ce735eb4fa9%2Fphp3k5qvx.png
Relevant equations: Coulomb's Law - E=kQ/r^2The attempt at a solution: Ok, so part I of this problem was to calculate the total charge of the rod, which I figured out easily enough. Part II, as stated above, is to find the electric field at some point P along the axis of the line of charge. Here's my attempted solution:

E = ∫ (kdQ/r^2)*<i> where dQ=ax^2dx where r=x. The x^2 on top and x^2 on bottom cancel out so you just end up integrating dx with bounds (D+L) and (L) and multiply by k and a. That didn't work, so I tried the equation with <xi> for the r vector and that didn't work either. I can't figure out what I'm doing wrong. Help!
 
Last edited:
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You need to integrate over the charge, from -L/2 to L/2. But the distance from the dq's to the point P is not the same as the x that "scans" the rod.
 

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