Half Wave Antenna Vector Potential Calculation?

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Vector Potential

Homework Statement


Consider two half wave antennas each ahving current

I(z,t)=\hat{z} I_{0}\cos\omega t\sin k(\frac{d}{2}-|z|)
where k=\omega/c
Each antenna has length d and points in the z direction. Antenna 1 is at (\Delta/2,0,0) and antenna two is at (-\Delta/2,0,0)

a) Find the vector potential A
b) Find the electric and magnetic field
c) Find dP/d\Omega
d) Evalute dP/d\Omega in the X Y plane when the antenna is seaparated by a distance lambda/2. Along what direction is the radiation preferentialy propagated?

Homework Equations


In CGS units so...
\vec{A}(\vec{r},t)=\frac{1}{c}\int \frac{\vec{J}(\vec{r},t_{r})}{|\vec{r}-\vec{r'}|} d\tau


The Attempt at a Solution


So we need the current as a function of z' and the retarded time

I(z,t)=\hat{z} I_{0}\cos\omega t\sin k(\frac{d}{2}-|z|)
I(z,t)=\hat{z} I_{0}\cos\omega (t-\frac{\mathcal{R}}{c})\sin k(\frac{d}{2}-|z|)

where \mathcal{R}=\sqrt{z'^2+r^2-2z'r\cos\theta}
since we want the fields far away (radiation zone), expand
\mathcal{R}\approx r\left(1-\frac{z'}{r}\cos\theta
so then
\cos\omega (t-\frac{\mathcal{R}}{c})\approx\cos\omega\left(t-\frac{r}{c}\left(1-\frac{z'}{r}\cos\theta\right)\right)
\cos\omega (t-\frac{\mathcal{R}}{c})\approx\cos\omega t \cos\frac{r}{c}\left(1-\frac{z'}{r}\cos\theta\right)+\sin\omega t\sin\frac{r}{c}\left(1-\frac{z'}{r}\cos\theta\right)

So then A is calculated like this? make the approximation that \mathcal{R}\approx r

\vec{A} = \hat{z}\frac{I_{0}}{rc}\int \sin k\left(\frac{d}{2}-|z|\right)\left(\cos\omega (t-\frac{\mathcal{R}}{c})\left(\cos\omega t \cos\frac{r}{c}\left(1-\frac{z'}{r}\cos\theta\right)+\sin\omega t\sin\frac{r}{c}\left(1-\frac{z'}{r}\cos\theta\right)\right) dz'

Ok since there are two antennas how should the integration be performed...
should i do for each antenna separately? That is integrate one of them from \Delta to \Delta+\frac{d}{2} and one of them from \Delta to \Delta-\frac{d}{2} ?? And then add the two results?

Thanks for your help!
 
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Since it is a radiation problem, I think you are allowed to assume r>>r' and
kr>>1, which greatly simplifies the problem.
 
To solve this, I first used the units to work out that a= m* a/m, i.e. t=z/λ. This would allow you to determine the time duration within an interval section by section and then add this to the previous ones to obtain the age of the respective layer. However, this would require a constant thickness per year for each interval. However, since this is most likely not the case, my next consideration was that the age must be the integral of a 1/λ(z) function, which I cannot model.
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