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C h a p t e r 2 0 : M i c r o w a v e W a v e g u i d e s a n d A n t e n n a s 451<br />

A. Operating frequency<br />

B. Increasing frequency<br />

C. Decreasing frequency<br />

/ 4<br />

a b c d<br />

/ 4<br />

/ 4<br />

/ 4<br />

a b c d<br />

/ 4<br />

/ 4<br />

"a"<br />

Dimension<br />

Figure 20.5 Changing frequency does not affect the<br />

analogy.<br />

On first glance, an explanation based<br />

on l/4 shorted stubs would seem to be<br />

valid only at one frequency. It turns out,<br />

however, that the analogy also holds up at<br />

other frequencies so long as the frequency<br />

is higher than a certain minimum cutoff frequency.<br />

The waveguide thus acts like a<br />

high-pass filter. Waveguides also have an<br />

upper frequency limit; between the upper<br />

and lower limits, waveguides support a<br />

bandwidth of 30 to 40 percent of the cutoff<br />

frequency. As shown in Fig. 20.5, between<br />

segments the centerline (which represents<br />

the conductors in the parallel line analogy)<br />

of the waveguide becomes a “shorting<br />

bar” that widens as the operating<br />

frequency gets higher and the l/4 stub on<br />

each side gets shorter or narrows as the<br />

operating frequency becomes lower and<br />

the l/4 stub lengthens.<br />

At the cutoff frequency, the fraction of<br />

the a dimension that acts as though it is a<br />

transmission line conductor is a minimum;<br />

in other words, the back-to-back<br />

l/4 stubs virtually touch at the midpoint<br />

of a. At this frequency, a = l/2. Above that<br />

frequency, the effective or apparent width<br />

of the conductor increases and l/2 < a.<br />

Below the cutoff frequency, the chamber<br />

ceases to function as a waveguide; instead,<br />

it acts like a conventional parallel transmission<br />

line with a pure reactance connected<br />

across the two conductors. Thus,<br />

the (low-frequency) cutoff frequency is defined<br />

as the frequency at which the a dimension<br />

is less than l/2.<br />

Propagation Modes in Waveguides<br />

Whether in a conventional transmission<br />

line or a microwave waveguide, the signal<br />

propagates as an electromagnetic wave,<br />

not as a longitudinal current. The transmission<br />

line supports a transverse electromagnetic<br />

(TEM) field. As explained in<br />

Chap. 3, the word transverse indicates that<br />

the wave is propagating at right angles to<br />

both the electric and the magnetic fields.<br />

In addition to the word transverse the

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