Practical_Antenna_Handbook_0071639586
456 P a r t V I : A n t e n n a s f o r O t h e r F r e q u e n c i e s line path (i.e., path ABC in Fig. 20.9B is longer than path AC). The relationship between c and V g is where v g = group velocity, in meters per second c = free-space velocity (3 × 10 8 m/s) a = angle of incidence in waveguide vg = c sin a (20.1) Clearly, v g can never be greater than c. The phase velocity is the velocity of propagation of the spot on the waveguide wall where the wave impinges (e.g., point B in Fig. 20.9B). Depending upon the angle of incidence, this velocity can actually be faster than both the group velocity and the speed of light! How can that be? Let’s look at an analogy. Consider an ocean beach, on which the waves arrive from offshore at an angle other than 90 degrees— in other words, the arriving wavefronts are not parallel to the shore. The arriving waves have a group velocity v g . But as a wave hits the shore, it will strike a point far down the beach first. Then the “point of strike” races up the beach at a much faster phase velocity v p , which is even faster than the group velocity. Similarly, in a microwave waveguide, the phase velocity can be greater than c, as can be seen from Eq. (20.2): v p c = sin a (20.2) Example 20.1 Calculate the group and phase velocities for an angle of incidence of 33 degrees. Solution (a) Group velocity (b) Phase velocity v g = c sin a 8 = (3× 10 )(sin 33°) 8 8 = (3× 10 )(0.5446) = 1.6 × 10 m / s v p = c / sin a 8 = (3× 10 m / s) / sin 33° 8 = (3× 10 m / s) / (0.5446) 8 = 5.51× 10 m / s
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 457 For this problem the solutions are 8 c = 3 × 10 m/s v v P g 8 = 5.51 × 10 m/s 8 = 1.6 × 10 m/s We can also write a relationship between all three velocities by combining Eqs. (20.1) and (20.2), resulting in c = v pv (20.3) g In any wave the product of frequency and wavelength is the velocity. Thus, for a TEM wave in unbounded free space we know that c = f l (20.4) fs Because the frequency f is fixed by the generator and the waveguide is a linear medium, only the wavelength can change when the velocity changes. In a microwave waveguide we can relate phase velocity to wavelength as the wave is propagated in the waveguide: v p λ × c = λ fs (20.5) where v p = phase velocity, in meters per second c = free-space velocity (3 × 10 8 m/s) l = wavelength in waveguide, in meters l fs = wavelength in free space (c/f ), in meters (see Eq. [20.4]) Equation (20.5) can be rearranged to find the wavelength in the waveguide: v l fs l = p (20.6) c Example 20.2 A 5.6-GHz microwave signal is propagated in a waveguide. Assume that the internal angle of incidence to the waveguide surfaces is 42 degrees. Calculate phase velocity, wavelength in unbounded free space, and wavelength in the waveguide.
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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 457<br />
For this problem the solutions are<br />
8<br />
c = 3 × 10 m/s<br />
v<br />
v<br />
P<br />
g<br />
8<br />
= 5.51 × 10 m/s<br />
8<br />
= 1.6 × 10 m/s<br />
<br />
We can also write a relationship between all three velocities by combining Eqs.<br />
(20.1) and (20.2), resulting in<br />
c = v<br />
pv<br />
(20.3)<br />
g<br />
In any wave the product of frequency and wavelength is the velocity. Thus, for a TEM<br />
wave in unbounded free space we know that<br />
c = f l<br />
(20.4)<br />
fs<br />
Because the frequency f is fixed by the generator and the waveguide is a linear medium,<br />
only the wavelength can change when the velocity changes. In a microwave<br />
waveguide we can relate phase velocity to wavelength as the wave is propagated in the<br />
waveguide:<br />
v<br />
p<br />
λ × c<br />
=<br />
λ<br />
fs<br />
(20.5)<br />
where v p = phase velocity, in meters per second<br />
c = free-space velocity (3 × 10 8 m/s)<br />
l = wavelength in waveguide, in meters<br />
l fs = wavelength in free space (c/f ), in meters (see Eq. [20.4])<br />
Equation (20.5) can be rearranged to find the wavelength in the waveguide:<br />
v l<br />
fs<br />
l = p (20.6)<br />
c<br />
Example 20.2 A 5.6-GHz microwave signal is propagated in a waveguide. Assume<br />
that the internal angle of incidence to the waveguide surfaces is 42 degrees. Calculate<br />
phase velocity, wavelength in unbounded free space, and wavelength in the waveguide.