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C h a p t e r 3 : A n t e n n a B a s i c s 103<br />

small region somewhere along either side of the dipole over the course of one complete<br />

cycle of RF energy from the transmitter.<br />

In Fig. 3.10A, standing voltage waveforms occurring at equal time intervals over<br />

the course of one cycle of RF energy are brought together on one axis, AB, corresponding<br />

to the total length of a half-wave antenna. As before, we assume that RF energy to<br />

drive the antenna is being injected at the center (point X).<br />

Figure 3.10B plots the standing voltage waveform as a function of time throughout<br />

one cycle of RF energy for two different points (A and Y) on the dipole. Note that the<br />

standing voltages seen at these two points are in phase—that is, their amplitudes go up<br />

and down simultaneously even though the peak amplitudes of the two points are, in<br />

general, different. This curve is valid for any pair of points or any number of points on<br />

the dipole.<br />

T 4<br />

T 4<br />

T 2<br />

T 6<br />

T 1<br />

T 7<br />

T<br />

Time 0<br />

T 8<br />

T 16<br />

A<br />

Y<br />

X<br />

B<br />

T 9<br />

T 15<br />

T 10<br />

T 14<br />

T 12<br />

T 12<br />

A<br />

Current distribution<br />

Current<br />

T 0 T 1 T 2 T 3 T 4 T 5 T 6 T 7 T 8 T 9 T 10 T 11 T 12 T 13 T 14 T 15 T 16<br />

Current at X<br />

Current at Y<br />

B<br />

Figure 3.11 Standing waves of current at two points on an antenna.

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