Lomion
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Can anyone tell me how to derive the equation for potential of an electric linear quadrupole?
http://img142.exs.cx/img142/8715/quadrupole3tj.jpg
My attempts yielded:
V = \frac{q}{4\pi\epsilon_0} [\frac{1}{R_1} - \frac{2}{R} + \frac{1}{R_2}]
V = \frac{q}{4\pi\epsilon_0} [\frac{RR_2 - 2R_1R_2 + RR_1}{RR_1R_2}]
Approximating with R >> d, I set RR_1R_2 = R^3
And I set R_1 = R-d\cos\theta and R_2 = R+d\cos\theta
Substituting in the equation, I get:
V = \frac{qd^2}{4\pi\epsilon_0R^3} [1+\cos{2\theta}]
However, the book's answer states that the potential
V = \frac{qd^2}{8\pi\epsilon_0R^3} [1+3\cos{2\theta}]
And I don't see how they got that. Was my approximation too inaccurate? Is there a geometric way to approximate this without going into taylor/maclaurin series expansion?
Thanks for any help offered!
http://img142.exs.cx/img142/8715/quadrupole3tj.jpg
My attempts yielded:
V = \frac{q}{4\pi\epsilon_0} [\frac{1}{R_1} - \frac{2}{R} + \frac{1}{R_2}]
V = \frac{q}{4\pi\epsilon_0} [\frac{RR_2 - 2R_1R_2 + RR_1}{RR_1R_2}]
Approximating with R >> d, I set RR_1R_2 = R^3
And I set R_1 = R-d\cos\theta and R_2 = R+d\cos\theta
Substituting in the equation, I get:
V = \frac{qd^2}{4\pi\epsilon_0R^3} [1+\cos{2\theta}]
However, the book's answer states that the potential
V = \frac{qd^2}{8\pi\epsilon_0R^3} [1+3\cos{2\theta}]
And I don't see how they got that. Was my approximation too inaccurate? Is there a geometric way to approximate this without going into taylor/maclaurin series expansion?
Thanks for any help offered!