The array-response of an antenna can be defined as:
A(Z)=N∑−NwnZn
where Z=exp(−iωΔt)=exp(−ikΔxsinα)
According to my textbook, if we let wn=1 for all n, the expression above can be written as:
A(Z)=sin[(2N+1)kΔxsinα/2](2N+1)sin[kΔxsinα/2]
where we have divded with (2N+1) so that A(1)=1
I tried to solve this algebraically to see how we get this expresison, but can't seem to figure it out. If we let wn=1 for all n, then we have:
A(Z)=N∑−NZn
which is a geometric series which can be expressed as:
A(Z)=Z−N−ZN+11−Z
However, I can't seem to get further than this. I tried plugging in z=exp(−ikΔxsinα) but only get a very complicated expression that I am unable to simplify. If anyone can give me any tips as to how to proceed with this derivation once I have obtained A(Z)=Z−N−ZN+11−Z, then I would be very grateful!
Answer
If we have wn=1, ∀n, you get
A(Z)=N∑n=−NZn=z−N2N∑n=0Zn=z−N1−z2N+11−z==z−(2N+1)/2−z(2N+1)/2z−1/2−z1/2
If you subsitute Z=exp(−ikΔxsinα) and divide by 2N+1 you finally get the expression given in your question.
(Of course you need to know that 2isinx=eix−e−ix).
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