Charge on Semicircle: Electric Field Equation

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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:
Diagram of a uniformly charged ring with point P on the axis above its center at height z, with distance r from P to the ring edge and radius R' shown. Labels give sigma as area charge density and lambda as linear charge density. Formula shown: E_z = k lambda 2 pi R' z / (z^2 + R'^2)^(3/2), with E_z arrow pointing upward at P.


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

[tex] <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 /> [/tex]
 
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.
 
Does this look reasonable:

[tex] <br /> \frac{Q}{4\pi \varepsilon_0(R^2 + Z^2)^{3/2} }(Z\hat{z}-R\hat{r})<br /> [/tex]
 
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.