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fluidistic
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Homework Statement
Two equal and opposite charges are attached to the ends of a rod of length s. The rod rotates counterclockwise at a speed ##\omega=ck##. The electric dipole moment of the system at ##t=0## is ##\vec p_0=qs\hat x##.
Show that the electric field in the radiation zone is ##\vec E_{\text{rad}}(r,\theta, \phi ,t)=\frac{k^2p_0}{4\pi\varepsilon_0}(\cos \theta \hat \theta +i\hat \phi )\frac{e^{i(kr-\omega t + \phi)}}{r}##.
(It's a part of a problem in Zangwill's book).
Homework Equations
[tex]\vec E _{\text{rad}}=\frac{\mu_0}{4\pi} \frac{\hat r (\hat r \cdot \ddot {\vec p} _{\text{ret}} - \ddot {\vec p}_{\text{ret}})}{r}[/tex]
The Attempt at a Solution
I tried the brute force approach by using the formula I just wrote above, in the relevant equations.
I got that ##\vec p (t)=p_0 [\cos (\omega t)\hat x + \sin (\omega t) \hat y]##.
So that [tex]\ddot {\vec p}_\text{ret}=p_0 \omega ^2 \{ -\cos \left [ \omega \left ( t-\frac{r}{c} \right ) \right ] \hat x -\sin \left [ \omega \left ( t-\frac{r}{c} \right ) \right ] \hat y \}[/tex]
Converting the Cartesian unit vectors to spherical unit vectors: ##\hat x =\sin \theta \cos \phi \hat r + \cos \theta \cos \phi \hat \phi -\sin \phi \hat \phi##. Plug and chug that into the formula for the E field... and I got a non vanishing ##\hat r## component which shouldn't happen.
I reached [tex]\frac{\mu_0 p_0 \omega ^2}{4\pi r}\{ -\sin \left [ \omega \left ( t-\frac{r}{c} \right ) \right ] \sin \theta \cos \phi +\cos \left [ \omega \left ( t-\frac{r}{c} \right ) \right ] \sin \theta \sin \phi +\cos \left [ \omega \left ( t-\frac{r}{c} \right ) \right ] \sin \theta \cos \phi +\sin \left [ \omega \left ( t-\frac{r}{c} \right ) \right ] \sin \theta \sin \phi \} \hat r[/tex]. I see I can factor out the sine of theta but I don't see how it's going to help me.
I don't seem to reach the desired result.
Any comment is welcome.Edit: Nevermind I see my error. I miscalculated ##\hat r \cdot \ddot {\vec p}_{\text{ret}}##. In fact I did ##\hat r \cdot \dot {\vec p}_{\text{ret}}##. I now get 0 for the ##\hat r## component as it should. Problem solved!
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