Practical_Antenna_Handbook_0071639586
Chapter 5 Antenna Arrays and Array Gain Multiple antennas or antenna elements fed from a common source of radiofrequency (RF) energy are collectively called an array. (Similarly, multiple antennas feeding a single receiver input also form an array.) The received signal at any distant point from an array of transmitting antennas is a combination of the signals from all the fed elements. Because each signal arriving at the receiving antenna has traveled a unique distance and its drive signal may have been phase-shifted with respect to others, the received signal is the vectorial combination of the contributions from all the elements of the array. Arrays are of interest because they make it possible, for a given transmitter power, to increase received signal strengths relative to a single radiating element. They are also important to understand because the effect of nearby earth or other conductors on the performance of antennas can often best be explained through array analysis. In this chapter we will explore the basics of arrays, using as our starting point all-driven arrays. All-Driven Arrays In Chap. 3 we saw that the strength of the received electromagnetic field far from a l/2 dipole or l/4 monopole transmitting (TX) antenna was proportional to the magnitude of the RF current at the feedpoint of the TX antenna. (See Fig. 5.1A.) The received signal will be a weak replica of the transmitted signal, delayed with respect to the original by an amount that will depend on the exact distance between the receiving and transmitting antennas. In simplified form, and ignoring the time it takes for the signal to reach the receiving point, the magnitude of the received E-field strength at a distant point is E RXorig = kI (5.1) TXorig I I = I TXorig ) ) ) ) ) Figure r r A E RXorig = KI TXorig 5.1A Received signal at a distant point from a single transmitting antenna. 149
150 p a r t I I : F u n d a m e n t a l s where E RXorig = field strength at distant receiving antenna I TXorig = feedpoint current of transmitting antenna k = constant that collects in a single number the total proportionality between E and I resulting from the specific characteristics of antennas, the orientation of the two antennas with respect to each other, and the attenuation along the path between them. Suppose we now excite a second transmitting antenna with feedpoint current I TXorig identical in all respects to the current in the first antenna; that is, a current having the same magnitude and phase (at the second feedpoint) as the first current. Further, let’s suppose we locate this second TX antenna at l/2 from the first but place it at exactly the same distance (Fig. 5.1B) from the receiving point so that the peak amplitudes of the two signals reach a maximum at the receive point at the same exact time. The principles of superposition and linearity tell us that the net, or total, received signal will now be twice that of the original because the receive antenna is intercepting two electromagnetic fields (that happen to be in phase) instead of one. Twice the current or voltage at the receiver input corresponds to a signal increase of 6 dB. (See App. A for an explanation of the use of logarithms and decibels to describe ratios of power, voltage, and current.) Now let’s cut the power to each of the two TX antennas in half, thus keeping the total power to the two antennas the same as the original power to the first TX antenna. At each TX antenna, then, P TXnew = ½ P TXorig . But since P = I 2 R, PTXnew ITXnew = (5.2) R where R is the feedpoint resistance of each antenna and I TXnew is the feedpoint current resulting from the new input power, P TXnew , to each element. Putting the old and the new equations for power in a ratio, we obtain for the new feedpoint current in each TX antenna I TXnew 2 P / 2 I R / 2 TXorig TXorig = = = ITXorig / 2 = 0.707I (5.3) TXorig R R 2 I 1 )))) I 1 = I 2 = I TXnew I 2 )))) Array axis r r r A E RXnew = 2KI TXnew Figure 5.1B Received signal at a distant point from two identical transmitting antennas.
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150 p a r t I I : F u n d a m e n t a l s<br />
where E RXorig = field strength at distant receiving antenna<br />
I TXorig = feedpoint current of transmitting antenna<br />
k = constant that collects in a single number the total proportionality<br />
between E and I resulting from the specific characteristics of antennas,<br />
the orientation of the two antennas with respect to each other, and the<br />
attenuation along the path between them.<br />
Suppose we now excite a second transmitting antenna with feedpoint current I TXorig<br />
identical in all respects to the current in the first antenna; that is, a current having the<br />
same magnitude and phase (at the second feedpoint) as the first current. Further, let’s<br />
suppose we locate this second TX antenna at l/2 from the first but place it at exactly the<br />
same distance (Fig. 5.1B) from the receiving point so that the peak amplitudes of the<br />
two signals reach a maximum at the receive point at the same exact time. The principles<br />
of superposition and linearity tell us that the net, or total, received signal will now be<br />
twice that of the original because the receive antenna is intercepting two electromagnetic<br />
fields (that happen to be in phase) instead of one. Twice the current or voltage at<br />
the receiver input corresponds to a signal increase of 6 dB. (See App. A for an explanation<br />
of the use of logarithms and decibels to describe ratios of power, voltage, and current.)<br />
Now let’s cut the power to each of the two TX antennas in half, thus keeping the<br />
total power to the two antennas the same as the original power to the first TX antenna.<br />
At each TX antenna, then, P TXnew = ½ P TXorig . But since P = I 2 R,<br />
PTXnew<br />
ITXnew<br />
= (5.2)<br />
R<br />
where R is the feedpoint resistance of each antenna and I TXnew is the feedpoint current<br />
resulting from the new input power, P TXnew , to each element.<br />
Putting the old and the new equations for power in a ratio, we obtain for the new<br />
feedpoint current in each TX antenna<br />
I<br />
TXnew<br />
2<br />
P / 2 I R / 2<br />
TXorig<br />
TXorig<br />
= = = ITXorig<br />
/ 2 = 0.707I<br />
(5.3)<br />
TXorig<br />
R R<br />
2<br />
I 1<br />
))))<br />
I 1<br />
= I 2<br />
= I TXnew<br />
I 2<br />
))))<br />
Array axis<br />
r<br />
r<br />
r <br />
A<br />
E RXnew<br />
= 2KI TXnew<br />
Figure 5.1B Received signal at a distant<br />
point from two identical transmitting<br />
antennas.