An infinitely long lossy transmission line with characteristic impeda...
As we know, the input impedance of infinitely long lossy transmission line is equal to its characteristic impedance. So, the input impedance to line 1 will be
Zin1 = Z01 = 200 Ω
From the shown arrangement of the transmission line, it is clear that the effective load impedance for line 2 will be equal to the input impedance of line 1.
i.e. ZL2 = Zin1 = 200 Ω
Since the length of the line 2 is λ/2, so the input impedance of line 2 will be equal to its load.
i.e. Zin2 = ZL2 = 200 Ω
(l = λ/2)
Therefore, the reflection coefficient at the load terminal of line 2 is given as
Now, the input voltage of line 2 is determined by using voltage division rule as
Again, the voltage at any point on line 2 is given as
whereV0+ is voltage of incident wave β is phase constant of the voltage wave and z is distance from load. So, for z = −λ/2
= – 2 volt
Therefore, the incident average power to the line 2 is given as
So, the reflected average power at the input terminal of line 1 (load terminal of line 2) is
Thus, we get the transmitted power to the line 1 as
Pavt = Pavi - Pavr = 20 - 2.2 = 17.8 m Watt