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a Matlab package for phased array beam shape inspection

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30 7 SNR ESTIMATE FOR THE TEST ARRAY<br />

6.2. Results<br />

b) Histogram of the <strong>beam</strong> direction change around the value θ 0<br />

∆θ = θ 0 trial − θ0 .<br />

The mean value and standard deviation of ∆θ over the trials is shown in line<br />

three of the plot header.<br />

c) Histogram of the <strong>beam</strong> width change from the computed value W 0 of the<br />

undistorted <strong>beam</strong>,<br />

∆W = W trial − W 0 .<br />

The mean value and standard deviation of ∆W over the trials is shown as<br />

the last item in line three of the plot header.<br />

Figures 21-24 show the <strong>beam</strong> <strong>shape</strong> jitter characteristics <strong>for</strong> a 50 × 20 element <strong>array</strong><br />

when the timing jitter at the elements varies from 100 ps to 1000 ps. In all cases, we<br />

assumed amplitude jitter 0.2 around the undistorted value of 1.0, (and normalized the<br />

amplitude power sum to unity). The <strong>beam</strong> width, in the xz-plane in this vertical pointing<br />

is W = 0.68 ◦ . This means that if we can accept 0.1 × W errors in pointing, in essentially<br />

no simulation run, should ∆W exceed 0.07 ◦ . The panel (b) of the figures show that<br />

this requirement clearly is fulfilled <strong>for</strong> timing jitter up to 500 ps, but starts to become<br />

questionable at the timing jitter of 1000 ps. The changes in <strong>beam</strong> width are similarly<br />

small up to about 500 ps.<br />

What is, perhaps, more troublesome is the loss of gain. At ∆t = 100 ps, the mean<br />

loss of gain in the main <strong>beam</strong> is about 10% (0.5 dB), at ∆t = 300 ps the loss is about<br />

25% (1.3 dB) and at 500 ps about 50% (3.0 dB).<br />

We emphasize that the loss of gain is mostly due to the “incohence” caused by the<br />

phase jitter. If we keep in the above four runs the input parameters otherwise intact but<br />

set the element amplitude jitter to zero, the <strong>beam</strong> jitter distributions change very little<br />

from those shown in Fig. 21-24. For example, the gain loss at 500 ps reduces from the<br />

50% to about 44%.<br />

Unless there is some fundamental problem with these simulation, it appears very clear<br />

that to get, say 0.1×<strong>beam</strong>width pointing accuracy, it is definitely enough to be able<br />

to control the element phase with something like 10–20 ◦ accuracy (clock timing with<br />

100–300 pc accuracy at 225 MHz), as long as the phase errors at individual elements are<br />

uncorrelated. The large number of elements (1000 in this simulation) then takes care<br />

about averaging the distortions so that the main effect is just some loss of gain. The<br />

randomness of the timing/phasing errors at the elements is so important that it perhaps<br />

should be en<strong>for</strong>ced.<br />

7. SNR estimate <strong>for</strong> the test <strong>array</strong><br />

To get a rough estimate of SNR <strong>for</strong> the Kiruna test <strong>array</strong>, assume that the test <strong>array</strong> is<br />

oriented towards the VHF antenna, long size (the x-direction) towards the VHF antenna,<br />

and that the VHF antenna is perpendicular to that direction, at x = L = 200 km in<br />

the test <strong>array</strong> coordinate system, and assume that the line from the test <strong>array</strong> to the<br />

VHF antenna is perpendicular to the VHF vertical direction (“flat Earth”), see Fig. 25.<br />

Also, assume optimal polarization matching and assume that the angle χ between the

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