Antenna Gain; Figure 1. Example Microwave Path With Parameters - ADTRAN 6000 Series System Manual

Section 2 Microwave Path Engineering Basics
Figure 1 illustrates a wireless link configuration containing all the parameters necessary for the power
budget analysis.
G
T
L
P
T
The following sections further discuss the power budget analysis and its components.

Antenna Gain

Actual transmit and receive antenna gain values depend strictly upon the physical characteristics of the
antennas installed for each link. In other words, the size of the dish determines the antenna gain. Using a
parabolic dish antenna results in the best performance. Antenna gains are specified in terms of decibels of
gain referenced to an isotropic source (dBi). An isotropic source is a hypothetical antenna having equal
radiation in all directions. The equation for calculating gain over isotropic radiation is
⎛
⎛
⋅ ⋅
⎜
G
10 log k
=
⎝
⎝
where
k dish efficiency factor (usually 0.55)
λ
carrier wavelength (c / f)
D dish diameter
The carrier wavelength (
measure. Use the same unit of measure for both variables. For example, a carrier
wavelength of 0.124 meters requires a dish diameter in meters as well.
The dish efficiency factor (k) is used to estimate how efficiently the dish reflector passes energy to the
feedhorn. The "standard" factor is 0.55 (measured performance of prime-focus dishes with a pyrimidal
waveguide feedhorn with no aperture blockage). Other dishes and feedhorn designs may have better or
worse efficiency. Table 1 on page 19 (standard) and Table 2 on page 19 (metric) provide gains using a 0.55
dish efficiency factor. Table 3 on page 19 (standard) and Table 4 on page 19 (metric) provide gains using a
0.40 dish efficiency factor. Dish manufacturers can provide gains for specific types of antennas.
18
λ

Figure 1. Example Microwave Path with Parameters

π D ⋅
⎞
2
⎞
⎟ (dBi)
----------- -
⎠
λ
⎠
λ
) and dish diameter (D) can be metric or standard units of
Copyright © 2005 ADTRAN, Inc.
TRACER 6000 Series Integrated System Manual
d, L
P
G
R
L
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