A standing wave of S = 4 is formed in free space(z < 0). The first maximum is observed at a distance 0.2[m] from the interface at z = 0 , and two adjacent maxima are found to be separated by 0.5[m]. Determine \eta _{2} of the material in the region z ≥ 0.
The distance between two adjacent maxima is equal to a half wavelength:
λ = 2 × 0.5[m] , and thus \beta _{1} = \frac{2 \pi }{\lambda } = 2\pi . (8-120)
The first maximum corresponds to n = 0 in Eq. (8-115b):
\boxed{z _{max} = – \frac{1}{2\beta _{1}} (\phi + 2\pi n)} (n = 0, ±1, ±2, …) (8-115b)
z _{max} = -\frac{1 }{2 \beta _{1} }\phi = – 0.2 [m] (8-121)
Inserting Eq. (8-120) into Eq. (8-121), we get
Φ = 0.8π (8-122)
From Eq. (8-119), we get
\boxed{S = \frac{\left|\hat{E}_{1}\right|_{max} }{\left|\hat{E}_{1}\right|_{min} } = \frac{1 + \left|\Gamma \right| }{1 – \left|\Gamma \right| } } (8-119)
\left|\Gamma \right| = \frac{S – 1}{S + 1} = \frac{4 -1}{4 + 1} = 0.6 (8-123)
Combining Eq. (8-122) and Eq. (8-123), the reflection coefficient is
\Gamma = 0.6 e^{j 0.8 \pi } (8-124)
Rewriting Eq. (8-107a), we have
\boxed{\Gamma = \frac{E^{r}_{o}}{E^{i}_{o}} = \frac{\eta _{2} – \eta _{1}}{\eta _{2} + \eta _{1}}} (8-107a)
\frac{\eta _{2}}{\eta _{1}} = \frac{1 + \Gamma }{1 – \Gamma } (8-125)
Substituting Eq. (8-124) and \eta _{1} = \eta _{o}= 377 [Ω] into Eq. (8-125), we get the intrinsic impedance of medium 2 as
\eta _{2}= 377 \frac{1 + 0.6 e^{j 0.8\pi } }{1 – 0.6 e^{j 0.8\pi } } = 154 e^{j 0.83} [\Omega ].