Graphics Programs Reference
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adopted. A two-dimensional (2-D) fan beam search pattern is shown in
Fig.1.15a.
In this case, the beamwidth is wide enough in elevation to cover the
desired search volume along that coordinate; however, it has to be steered in
azimuth.
Figure 1.15b
shows a stacked beam search pattern; here the beam has
to be steered in azimuth and elevation. This latter kind of search pattern is nor-
mally employed by phased array radars.
Search volumes are normally specified by a search solid angle in steradi-
ans. Define the radar search volume extent for both azimuth and elevation as
and
Ω
. Consequently, the search volume is computed as
Θ
A
Θ
E
)
2
Ω
A
Θ
E
=
(
)
⁄
(
57.296
steradians
(1.61)
where both and are given in degrees. The radar antenna beam-
width can be expressed in terms of its azimuth and elevation beamwidths
Θ
A
Θ
E
3
dB
θ
a
and
, respectively. It follows that the antenna solid angle coverage is
θ
e
θ
a
θ
e
and, thus, the number of antenna beam positions
required to cover a solid
n
B
angle
is
Ω
Ω
n
B
=
--------------------------------------------
(1.62)
)
2
(
θ
a
θ
e
)
⁄
(
57.296
In order to develop the search radar equation, start with Eq. (1.56) which is
repeated here, for convenience, as Eq. (1.63)
P
t
G
2
λ
2
σ
4(
3
kT
e
BFLR
4
SNR
=
-----------------------------------------
(1.63)
Using the relations
and
, where
is the PRI and
is
τ
=
1
⁄
B
P
t
=
P
av
T
τ
⁄
T
τ
the pulsewidth, yields
P
av
G
2
λ
2
στ
4(
3
kT
e
FLR
4
T
---
-------------------------------------
SNR
=
(1.64)
(a)
(b)
Figure 1.15. (a) 2-D fan search pattern; (b) stacked search pattern.
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