Beamwidth, near/far field

07mar19


Some conversion factors:


Near, far field and the sky ovverlap at 100 km.  (top)

    The illuminated area on the dish (and the edge taper) determine the half power beam width (HPBW) at a given frequency.The relationship is:       In the far field,  rays from opposite sides of the dish to a point in the far field are parallel. For points in the near field, the rays are not parallel. We can define parallel by the path difference being less than a fraction of a wavelength.

     The path difference for rays from the opposite edges of the dish to a point P is:

point P phase diff to center and
        edge of dish

 
We can define the near, far field transition as the height were dl is a fraction of a wavelength:

dl=lambda/n = D^2/(8*H)
H=D^2/(8*lambda/n)

Some values are:

wavelength difference at P
h
lambda/4
D^2/(2*lambda)
lambda/8
D^2/lambda
lambda/16
2*D^2/lambda


The table below  shows the transition region for some arecibo frequencies for different values of dl

Htrans=D**2/(8*lamba/N)
freq (Mhz)
Lambda (m)
Transition Region (Km)
diam=305m

diam=225m
dl=lambda/8
dl=lambda/16
dl=lambda/8 dl=lambda/16
327
0.917
101
202
55
110
430
0.697
133
267
72
145
1300
0.230
403
806
219
438
2380
0.126
738
1476
401
803
5000
0.060
1550
3100
843
1687
7000
0.043
2171
4341
1181
2362
9000
0.033
2791
5581
1518
3037



Using the hpbw to define the illuminated area (d=k*lambda/hpbw)  and solving for H gives:

see also: ../430yagi/yagi/deltaPhase.xfig, ./nearfarfield.pro

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