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a Matlab package for phased array beam shape inspection

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52 A FIGURES TO CHAPTERS 2–7<br />

1<br />

2 3 4<br />

1<br />

2 3<br />

u y<br />

0<br />

5 1 6<br />

u y<br />

0<br />

4 1 5<br />

7 8 9<br />

6 7<br />

−1<br />

−1<br />

−1 0 1<br />

−1 0 1<br />

u x<br />

u x<br />

(a) θ 1 = 4.0 ◦ , g 4 = g 9 = -23 dB<br />

(b) θ 1 = 5.0 ◦<br />

Grating<br />

1<br />

2 3 4<br />

1<br />

2 3<br />

u y<br />

0<br />

5 1 6<br />

u y<br />

0<br />

4 1 5<br />

7 8 9<br />

6 7<br />

−1<br />

−1<br />

−1 0 1<br />

−1 0 1<br />

u x<br />

u x<br />

(c) θ = 4.0 ◦ , g 4 = g 9 = -11 dB<br />

(d) θ 1 = 5.0 ◦<br />

Figure 20: Explaining the directivity dips. This figure illuminates the origin of the dip<br />

at θ ≈ −4.5 ◦ in the directivity curves of Fig. 19. In panels (a) and (b), the<br />

<strong>array</strong> elements are vertical, in panels (c) and (d), the elements have been<br />

tilted to φ E = 0, θ E = 40 ◦ . When the marker <strong>beam</strong> (<strong>beam</strong> 1) is phase-steered<br />

from 4 ◦ to 5 ◦ , two grating <strong>beam</strong>s move out of the circle of visibilitity. For the<br />

tilted elements, a still significant amount of power is suddenly taken and then<br />

re-released, <strong>for</strong> the gain of both the horizontal <strong>beam</strong>s is still only about 10 dB<br />

down from the main <strong>beam</strong>s. Instead, <strong>for</strong> the vertical elements, <strong>beam</strong>s 4 and<br />

9 have so little gain that what they do near the boundarary of the visibility<br />

circle does not matter in the power budget. The figure was produces with<br />

plane<strong>array</strong>.

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