Charge on Semicircle: Electric Field Equation

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The discussion focuses on the electric field generated by a charge distributed along a semicircle compared to a full ring. It highlights that the absence of opposing forces in a semicircle alters the symmetry, affecting the electric field calculations. The vertical component of the electric field remains straightforward to compute, but the horizontal component requires a separate integral due to the broken symmetry. Participants emphasize the need for clarity in calculations and suggest that showing complete work would help identify errors. Overall, the conversation revolves around the complexities of integrating electric field components for a semicircular charge distribution.
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Homework Statement


This is not a homework problem so there is no problem statement. More of a conceptual question.

Consider a charge on a ring:
eler3.gif


If this was a semicircle opposed to a ring, how would this change the equation since there is not an opposing dEr force.

<br /> <br /> \boldsymbol{E} = \boldsymbol{\hat{z}} \frac{\rho_l R(-\hat{\boldsymbol{r}}R + \hat{\boldsymbol{z}Z})}{4 \pi \varepsilon_0 (R^2 + Z^2)^{3/2}}\int_{0}^{\pi }d\phi <br /> <br />
 
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The vertical component is still easy to calculate (as you just have a smaller part of the ring contributing to it), but the other component (due to the broken symmetry it does not vanish any more) will need its own integral. No idea how easy/messy that gets.
 
So I would have to do it twice.

dE = dEr + dEz
 
The integrals are different, but yes.
 
Does this look reasonable:

<br /> <br /> \frac{Q}{4\pi \varepsilon_0(R^2 + Z^2)^{3/2} }(Z\hat{z}-R\hat{r})<br /> <br />
 
Z and z are the same?

That would mean the electric field points in the same direction as the "r" line in the sketch. No, that cannot work.
It would be easier to find the error if you show your whole work.
 
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