Correct Answer - Option 4 : 150 ohm
Concept:
\({{Z}_{in}}={{Z}_{0}}\left( \frac{{{Z}_{L}}+j{{Z}_{0}}\tan \beta l}{{{Z}_{0}}+j{{Z}_{L}}\tan \beta l} \right)\)
\(\because \beta =\frac{2\pi }{\lambda }\), at a quarter \(\left( \frac{\lambda }{4} \right)\) distance away,
\({{Z}_{in}}={{Z}_{0}}\frac{\left( {{Z}_{L}}+j{{Z}_{0}}\tan \left( \frac{2\pi }{\lambda }.\frac{\lambda }{4} \right) \right)}{\left( {{Z}_{0}}+j{{Z}_{L}}\tan \left( \frac{2\pi }{\lambda }.\frac{\lambda }{4} \right) \right)}\)
\({{Z}_{in}}=\frac{Z_{0}^{2}}{{{Z}_{L}}}\)
Calculation:
Given, ZL = 225 Ω
Zin = 100 Ω
\({{Z}_{in}}=\frac{Z_{0}^{2}}{{{Z}_{L}}}\)
Putting on the respective values and solving for Z0, we get:
Z02 = Zin × ZL
Z02 = 100 × 225 = 22500
Z0 = 150 Ω
So the quarter-wave transformer should have a characteristic impedance of 150 Ω.