8. Rectangular Patch Antenna
β’ The length of the patch is:
π0
3
< πΏ <
π0
2
β’ At low frequencies, initial vales of π πeff. referred to as the static values and are
given by:
π πeff. =
π π
+1
2
+
π π
β1
2
[1+
12β
π€
]-1/2
Where,
h= height of substrate
w= width of the patch
9. Rectangular Patch Antenna
β’ For an efficient radiator, practical width that leads to good radiator
efficiencies is:
W =
1
2ππ π0
π0
2
π π
+1
=
π£0
2ππ
2
π π
+1
β’ For normalized extension of length:
βπΏ
β
= 0.412
(π πeff.+0.3)(
π
β
+0.264)
(π πeff.β0.258)(
π
β
+0.8)
Where,v0= free space velocity of light
10. Rectangular Patch Antenna
β’ Directivity of the single patch is:
D0 = {5. 2dB W<<π0
4(
π
π0
) W>>π0
β’ Finally, the effective length of the patch is:
Leff. = L+2 βπΏ
Where, βπΏ= extended length of the patch
11. Rectangular Patch Antenna
β’ The actual length of the patch can be determined by solving:
L =
1
2ππ π πeff. π0
π0
- 2 βπΏ
β’ Finally, the effective length of the patch is:
Leff. = L+2 βπΏ
Where, βπΏ= extended length of the patch
12. Remedies:
β’ Low power and low gain can overcome by arrays
configuration.
β’The band width can increase up to 60% by using some
special techniques.
β’Surface wave associated limitations such as poor
efficiency,increased mutual coupling , reduced gain and
radiation pattern can overcome.