Field Due to Continuous Distribution of Charge

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Homework Help Overview

The problem involves calculating the Coulomb force between two line charges represented by rods with specified lengths and charge densities, positioned along the x-axis with a defined separation distance. The focus is on determining the electric field generated by one rod at the location of the other rod.

Discussion Character

  • Exploratory, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • The original poster attempts to derive the electric field at a point near the second rod using integration, expressing the field in terms of the charge density and distance.
  • Some participants question the correctness of the original poster's expression for the electric field, suggesting that certain variables may be missing or misdefined.
  • There is a discussion about the interpretation of distance variables and their relation to the positions of the rods.

Discussion Status

Participants are actively engaging in clarifying the setup of the problem and the expressions used for the electric field. Some guidance has been offered regarding the integration limits and the formulation of the electric field, but no consensus has been reached on the original poster's approach.

Contextual Notes

There is an emphasis on ensuring that the distances used in the calculations accurately reflect the physical setup of the problem, with specific attention to the positions of the rods and the points of interest for calculating the electric field.

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Homework Statement



Coulomb force between line charges: a rod of length l1 with line charge density λ1 and a rod of length l2 with line charge density λ2 lie on the x axis. Their ends are separated by a distance D as shown in the figure.

(a) What is the force F between these charges?

diagram: http://ocw.mit.edu/NR/rdonlyres/Physics/8-022Fall-2004/3A772032-6B74-4D2D-A550-8F0ECFECEDBC/0/pset1.pdf

#7


Homework Equations



E = [tex]\frac{1}{4\pi\epsilon}[/tex][tex]\int\frac{dq}{r^2}[/tex]
F = [tex]\int E dq[/tex]



The Attempt at a Solution


So, first I decided to find the field at a point a distance D from the end of line 1. Using the standard x coordinate system, I placed line 1 such that its endpoints are 0, [tex]l_{1}[/tex].

E = [tex]\frac{1}{4\pi\epsilon}[/tex][tex]\int\frac{dq}{r^2}[/tex]

Limits of integration being (0,

Using this and dq = [tex]dl_{1}[/tex][tex]\lambda_{1}[/tex], all I need to do is find a function for r in terms of l, which is the distance from 0. Which would be ([tex]l_{1}[/tex] + D) - l.

I renamed ([tex]l_{1}[/tex] + D) as the variable a to make the integration simpler. So now I have:

E = [tex]\frac{\lambda_{1}}{4\pi\epsilon}[/tex][tex]\int \frac{dl}{(a - l)^2}[/tex]

which is just [tex]\frac{\lambda_{1}}{4\pi\epsilon} *[/tex][tex]\frac{1}{a-l_{1}}[/tex]

and because a = d + [tex]l_{1}[/tex]

I get the E Field being E = [tex]\frac{\lambda_{1}}{4d\pi\epsilon}[/tex]

Is this correct so far? Clearly my success on the second part depends on that because all I have to do is just integrate the field over the infinitesimal segments of charge over the second line's length yes? And to find that distance d as a function of l it's just ( l - length 1), where l is the distance from the 0 point. I'm just kind of shaky on the first part, finding the field, that's all.
 
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In the expression of E at the starting point of l2, the distance l1 must appear which is missing in your expression.
Try this one.
dE = k*lambda1*dx/(D+x)^2.
Integrate it from x = 0 to x = l1 and find E.
 
Wait, is x the distance from l1? Because then D + x is the distance from some point on the line to P2 which is what i want. Because my expression actually has d in it? It's just "a" is in terms of D, and i defined my distance variable as from x = 0. I'm not sure, it looks like x+d only works if x is the distance from l1. Or am I misunderstanding something here?
 
You want to find the field due to rod1 at the starting point of rod 2.
So E = k*lambda1*[-(1/(x+D)]. Find the value of E taking the limits from x = D to x= (l1 +D)
 

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