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A long overhead transmission line is terminated by its characteristic impedance. Under this operating condition, the ratio of the voltage to the current at different points along the line will
Progressively increase from the sending-end to the receiving-end
Progressively increase from the receiving-end to the sending-end
Remain the same at the two ends, but is higher between the two end being maximum at the centre of the line
Remain the same at all points
Remain the same at all points
Quick Summary: When a transmission line is terminated by its characteristic impedance $Z_0$, the line is said to be 'matched'. Under this condition, there is no reflected wave, and the ratio of voltage to current is constant at every point along the line, equal to $Z_0$.
When a transmission line is terminated by its characteristic impedance Z0тАЛ, the line is said to be 'matched'. Under this condition, there is no reflected wave, and the ratio of voltage to current is constant at every point along the line, equal to Z0тАЛ.
Z0тАЛ=G+j╧ЙCR+j╧ЙLтАЛтАЛ тАФ characteristic impedance of a transmission line
I(x)V(x)тАЛ=Z0тАЛ тАФ constant ratio when terminated by Z0тАЛ
The voltage and current at any point x on a lossy transmission line are given by V(x)=V+eтИТ╬│x+VтИТe╬│x and I(x)=Z0тАЛV+тАЛeтИТ╬│xтИТZ0тАЛVтИТтАЛe╬│x. If the line is terminated by ZLтАЛ=Z0тАЛ, the reflection coefficient ╬У=ZLтАЛ+Z0тАЛZLтАЛтИТZ0тАЛтАЛ becomes zero, meaning VтИТ=0. Consequently, the ratio I(x)V(x)тАЛ=Z0тАЛ remains constant regardless of the position x.
Matched termination prevents reflections on the line.
A matched line behaves as if it were infinitely long.
The input impedance of a matched line is independent of the line length.
Maximum power transfer occurs when source impedance equals characteristic impedance.
Elimination of standing waves
Prevention of signal reflection/distortion
Not always possible due to varying load conditions
Requires impedance matching networks for non-ideal loads
RF transmission lines
Telecommunication cabling
Pulse power systems
If ZLтАЛюАа=Z0тАЛ, standing waves are formed, and the ratio V/I varies as a function of the distance from the load.
Option D is the correct physical interpretation of a matched transmission line.
D is correct тАФ Because the line is terminated by its characteristic impedance, no reflection occurs, ensuring the voltage-to-current ratio remains constant at Z0тАЛ throughout the line length.
Always remember that a line terminated in Z0тАЛ is 'electrically invisible' to the source; it simply looks like a fixed resistor Z0тАЛ regardless of the line length.