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ElectricalPower System
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For distortion less transmission line

A

RL=GCRL = GCRL=GC

B

RC=GLRC = GLRC=GL

C

RG=LCRG = LCRG=LC

D

RLGC=0RLGC = 0RLGC=0

Correct Answer

тЪЩя╕П TE тАв Technical Concept & PrincipleElectricalPower System
Option B

RC=GLRC = GLRC=GL

Quick Summary:

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=GLRC = GLRC=GL, which ensures that the signal maintains its waveform shape during propagation.

тЪЩя╕ПTETechnical SolutionConcept & Principle
ЁЯТб Explanation

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=GLRC = GLRC=GL, which ensures that the signal maintains its waveform shape during propagation.

ЁЯФв Key Formulas

╬│=(R+j╧ЙL)(G+j╧ЙC)\gamma = \sqrt{(R + j\omega L)(G + j\omega C)}╬│=(R+j╧ЙL)(G+j╧ЙC)тАЛ тАФ General propagation constant

RC=GLRC = GLRC=GL тАФ Distortionless condition

╬▒=RG\alpha = \sqrt{RG}╬▒=RGтАЛ тАФ Attenuation constant (frequency independent)

╬▓=╧ЙLC\beta = \omega\sqrt{LC}╬▓=╧ЙLCтАЛ тАФ Phase constant

тЪЩя╕П Working Principle

The propagation constant is defined as ╬│=(R+j╧ЙL)(G+j╧ЙC)\gamma = \sqrt{(R + j\omega L)(G + j\omega C)}╬│=(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., RL=GC\frac{R}{L} = \frac{G}{C}LRтАЛ=CGтАЛ. This condition simplifies the expression for ╬│\gamma╬│ such that ╬▒=RG\alpha = \sqrt{RG}╬▒=RGтАЛ (frequency independent) and ╬▓=╧ЙLC\beta = \omega\sqrt{LC}╬▓=╧ЙLCтАЛ (linear phase shift).

ЁЯУМ Key Points
  • тЦ╕

    Distortionless lines eliminate both frequency and phase distortion.

  • тЦ╕

    The attenuation constant ╬▒\alpha╬▒ remains constant with respect to frequency.

  • тЦ╕

    The phase velocity vp=1LCv_p = \frac{1}{\sqrt{LC}}vpтАЛ=LCтАЛ1тАЛ becomes independent of frequency.

  • тЦ╕

    These lines are theoretically ideal but practically difficult to achieve for all frequencies.

тЬЕ Advantages
  • тЦ╕

    Preserves the waveform shape of the signal

  • тЦ╕

    Constant time delay for all signal components

тЭМ Disadvantages / Limitations
  • тЦ╕

    Hard to implement in practice as it requires specific R, L, G, C values

  • тЦ╕

    Often requires artificial loading (loading coils)

ЁЯЫая╕П Applications / Uses
  • тЦ╕

    Long distance telegraphy

  • тЦ╕

    High-speed data communication lines

ЁЯУД Additional Information
  • тЦ╕

    The condition RC=GLRC = GLRC=GL implies that the time constants of the series and shunt branches are identical.

  • тЦ╕

    Option A (RL=GC) is incorrect as it represents an incorrect algebraic arrangement of parameters.

ЁЯУК Diagram / Illustration
Distortionless ConditionR / L = G / CRC = GL
тЬЕ

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=GLRC = GLRC=GL.

Core Concepts Used
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Transmission Line Theory Distortionless Lines Propagation Constant
ЁЯТб EXAM TIP

Remember that for a lossless line (R=0,G=0R=0, G=0R=0,G=0), the distortionless condition is automatically satisfied, which is a specific case of the general RC=GLRC=GLRC=GL condition.

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