What is the Electric Field at a Point Near an Infinite Line of Charge?

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SUMMARY

The discussion focuses on calculating the electric field at a point near an infinite line of charge with a uniform charge distribution of λ = -2.3 μC/m. The user initially attempts to use the formula E = 2kL / r, which is inappropriate for this scenario. Instead, the correct approach involves setting up an integral for the electric field contributed by an element of charge, specifically ∫(0 to ∞) kλ/(y+3)^2 dy. This integral accounts for the contributions of the electric field from the entire line of charge.

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TwinGemini14
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An infinite line of negative charge begins at the origin and continues forever in the +y-direction. It has a uniform charge distribution of λ = -2.3 μC/m. Calculate the x and y-component of the electric field at the point (0,-3 m).

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So immediately realized that Ex = 0 since te charge also lies on the y axis. I cannot seem to evaluate what Ey would be.

L=Lambda

Here's what I'm doing: E = 2kL / r
E = 2(9*10^9)(-2.3*10^-6) / (-3)
E = 13800 N/C

What am I doing wrong? Can somebody please help me? I've been working on this problem for a very long time. Thanks in advance.
 
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TwinGemini14 said:
Here's what I'm doing: E = 2kL / r
That formula describes the field surrounding an infinite line of charge at some distance (r) from the line. Not useful for this problem since you are finding the field along the line of the charge and you are dealing with the end of the line of charge. Instead, set up an expression for the field contributed by an element of charge and integrate.
 
I don't understand how to set up this integral. Will the limits be from 0 to infinity?

inf.
k | (-2.3*10^-6)y / (3+y)^2
0


| = integrand

Does this look right? I seriously do not understand how to set up this equation. Help please!
 
TwinGemini14 said:
inf.
k | (-2.3*10^-6)y / (3+y)^2
0
That's pretty close. Here's how I would write it:

(0 to ∞) kλ/(y+3)^2 dy

Forget the sign of the charge, just worry about the magnitude. You'll assign the proper direction and sign to the field at the end.
 

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