Electric field of a uniformly distributed rod

AI Thread Summary
The discussion focuses on calculating the electric field at a point on the x-axis due to a uniformly distributed rod with opposing charges on either side. The user derives the expression for the electric field using integration and symmetry, resulting in E = 2KQ/a[1/x^2 - 1/(x-a)^2]. Questions arise regarding the correctness of the integration and the application of symmetry, particularly in how to handle the limits of integration and the multiplication by two. The user seeks clarification on transitioning to the second Taylor expansion term for the case where x is much greater than a. The conversation emphasizes the importance of verifying assumptions and integration steps in electrostatics problems.
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Homework Statement


rod -a-------|---------a on x-axis, for x>-a has -Q charge, for X<a has +Q charge, find the electric field at point (x,0) x is positive


Homework Equations


lambda = Q/a linear charge density dQ = (lambda)(ds)
E=KQ/r^2

The Attempt at a Solution


i make dE=kdQ/(x-s)^2
integrate kdQ/(x-s)^2 between -a and a ( i can make it 0 to a and multiply by two, symmetry)
i get the result 2KQ/a[1/x^2 - 1/(x-a)^2] for E sub-x

now if i want to find x>>a i need o somehow change [1/x^2 - 1/(x-a)^2] to the 2nd taylor expansion term but how? And is my integration correct?
 
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I suggest checking the assumption about symmetry.
 
I don't understand how you multiplied by 2... you have the integral:

\int_{-a}^{0}\frac{k\sigma ds}{(x-s)^2} + \int_{0}^{a}\frac{-k\sigma ds}{(x-s)^2}

where sigma is Q/a
 
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