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For distortion less transmission line
RL=GC
RC=GL
RG=LC
RLGC=0
RC=GL
A transmission line is considered distortionless if the attenuation constant is independent of frequency and the phase velocity is constant for all frequencies. This occurs when the transmission line parameters satisfy the condition RC=GL, which ensures that the signal maintains its waveform shape during propagation.
A transmission line is considered distortionless if the attenuation constant is independent of frequency and the phase velocity is constant for all frequencies. This occurs when the transmission line parameters satisfy the condition RC=GL, which ensures that the signal maintains its waveform shape during propagation.
╬│=(R+j╧ЙL)(G+j╧ЙC)тАЛ тАФ General propagation constant
RC=GL тАФ Distortionless condition
╬▒=RGтАЛ тАФ Attenuation constant (frequency independent)
╬▓=╧ЙLCтАЛ тАФ Phase constant
The propagation constant is defined as ╬│=(R+j╧ЙL)(G+j╧ЙC)тАЛ. For distortionless lines, the ratio of the series impedance to the shunt admittance must be equal to the ratio of resistance to conductance, i.e., LRтАЛ=CGтАЛ. This condition simplifies the expression for ╬│ such that ╬▒=RGтАЛ (frequency independent) and ╬▓=╧ЙLCтАЛ (linear phase shift).
Distortionless lines eliminate both frequency and phase distortion.
The attenuation constant ╬▒ remains constant with respect to frequency.
The phase velocity vpтАЛ=LCтАЛ1тАЛ becomes independent of frequency.
These lines are theoretically ideal but practically difficult to achieve for all frequencies.
Preserves the waveform shape of the signal
Constant time delay for all signal components
Hard to implement in practice as it requires specific R, L, G, C values
Often requires artificial loading (loading coils)
Long distance telegraphy
High-speed data communication lines
The condition RC=GL implies that the time constants of the series and shunt branches are identical.
Option A (RL=GC) is incorrect as it represents an incorrect algebraic arrangement of parameters.
B is correct тАФ A transmission line is distortionless if the ratio of its series resistance to inductance equals the ratio of its shunt conductance to capacitance, expressed as RC=GL.
Remember that for a lossless line (R=0,G=0), the distortionless condition is automatically satisfied, which is a specific case of the general RC=GL condition.