hi freind
We combine the gain of the transmitting antenna with the effective area of the receiving
antenna to determine delivered power and path loss.
the path loss:
Pd/Pt= A
2G
1(ƒÆ, ƒÓ)/(4ƒÎR
2)
Antenna 1 transmits, and antenna 2 receives. If the materials in the antennas are
linear and isotropic, the transmitting and receiving patterns are identical (reciprocal) [2,
p. 116]. When we consider antenna 2 as the transmitting antenna and antenna 1 as the
receiving antenna, the path loss is
Pd/Pt= A
1G
2(ƒÆ, ƒÓ)/(4ƒÎR
2)
Since the responses are reciprocal, the path losses are equal and we can gather and
eliminate terms:
G1/A1= G2/A2= constant
Because the antennas were arbitrary, this quotient must equal a constant. This constant
was found by considering the radiation between two large apertures
G/A= 4ƒÎ/ƒÉ
2We substitute this equation into path loss to express it in terms of the gains or effective
areas:
Pd/Pt= G
1G
2(ƒÉ/(4ƒÎR))
2= A
1A
2/(ă
2R
2)
We make quick evaluations of path loss for various units of distance R and for frequency
f in megahertz using the formula
path loss(dB) = K
U + 20 log(fR) − G
1(dB) − G
2(dB)
where K
U depends on the length units:
Unit K
U---------------
km 32.45
nm 37.80
miles 36.58
m −27.55
ft −37.87
Example Compute the gain of a 3-m-diameter parabolic reflector at 4 GHz assuming
55% aperture efficiency.
Gain is related to effective area by
G = 4ƒÎA/ƒÉ
2We calculate the area of a circular aperture by A = ƒÎ(D/2)
2. By combining these equations, we have
G =(ƒÎD/ƒÉ)
2ā
a =(ƒÎDf/c)
2ā
awhere D is the diameter and ā
a is the aperture efficiency. On substituting the values
above, we obtain the gain:
G =[3ƒÎ(4 ~ 10
9)/(0.3 ~ 10
9)]
2(0.55) = 8685 (39.4dB)
enjoy