What is the electric field at the end of a thin rod with a distributed charge?

AI Thread Summary
The discussion focuses on calculating the electric field at the end of a thin rod with a distributed charge, where the charge density is proportional to the square of the distance from one end. The user struggles with integrating the electric field due to the variable charge density and determining the constant k. Clarifications are provided that the total charge must be calculated to find k, and a mistake in relating charge density to total charge and length is pointed out. The importance of using the correct constant in Coulomb's Law is emphasized, suggesting the use of 1/(4πε₀) instead of k. The conversation concludes with encouragement to think critically about the problem.
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Homework Statement



Thin rod AB has length l=100 cm and total charge q0=37 nC that is distributed in such a way that its line density λ is proportional to the square of the distance from the end A, i.e. λ(x) =kx2. Determine electric field E at the end A of the rod.

Homework Equations



E = kq/r^2, λ = Q/l, dq = λdl

The Attempt at a Solution



I tried doing substituting the line density into the integral of the electric field making: dE = kλdl/r^2 and then I get stuck because if I try to make r = x then the line density will cancel with the x^2 and leaving just the K and I don't know what K is or how to solve for it. If someone can help me with this problem it would be greatly appreciated. Thanks!
 
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You are told explicitly, \lambda = kx^2
So stating \lambda =\frac{Q}{\ell} is a mistake!

The total charge is a quantity you need to determine the numerical value of k
 
RoyalCat said:
You are told explicitly, \lambda = kx^2
So stating \lambda =\frac{Q}{\ell} is a mistake!

The total charge is a quantity you need to determine the numerical value of k

Oh okay. Then if dE = kλdx/r^2, is it valid to say that r = l/2 to have dE = kλdx/(l^2/4) the integral from 0 to l? How are we suppose to find the value of k if we can't relate the λ with Q and l?
 
You know that \frac{dq}{dx}=\lambda
Therefore, Q_{total}=\int^{\ell}_0 \lambda dx
 
Last edited:
So therefore Q total = l which is 100cm so then k in λ=kx^2 equals 100? Also how does that help me simply the integral from 0 to l of dE = kλdx/r^2?
 
Due to a typo in the TeX, the lambda didn't show up in the integral. Don't take everything you're told by fiat. Think things through. What I posted earlier was nonsense. I said that the total charge is the length of the rod. That's gibberish.

Please think the problem through, I've given you all the help you should require. Just on a final note, I suggest you use \frac{1}{4\pi\epsilon_0} for the constant in Coloumb's Law, since k is already taken, and has a different meaning in this exercise.
Best of luck. :)
 
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