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ElectricalPower System
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Reflection coefficient at the load end of short circuited line is

A

Zero

B

10┬░

C

190┬░

D

180┬░

Correct Answer

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

180┬░

Quick Summary:

The reflection coefficient (╬У\Gamma╬У) at the load end is defined by the ratio of the reflected voltage wave to the incident voltage wave. For a short-circuited load, the load impedance is ZL=0Z_L = 0ZLтАЛ=0, which results in a reflection coefficient of тИТ1-1тИТ1, corresponding to a phase shift of 180┬░180┬░180┬░.

тЪЩя╕ПTETechnical SolutionConcept & Principle
ЁЯТб Explanation

The reflection coefficient (╬У\Gamma╬У) at the load end is defined by the ratio of the reflected voltage wave to the incident voltage wave. For a short-circuited load, the load impedance is ZL=0Z_L = 0ZLтАЛ=0, which results in a reflection coefficient of тИТ1-1тИТ1, corresponding to a phase shift of 180┬░180┬░180┬░.

ЁЯФв Key Formulas

╬У=ZLтИТZ0ZL+Z0\Gamma = \frac{Z_L - Z_0}{Z_L + Z_0}╬У=ZLтАЛ+Z0тАЛZLтАЛтИТZ0тАЛтАЛ тАФ General formula for reflection coefficient

╬Уsc=тИТ1\Gamma_{sc} = -1╬УscтАЛ=тИТ1 тАФ Reflection coefficient for short-circuited line

тЪЩя╕П Working Principle

When a traveling wave reaches a short circuit, the boundary condition requires the total voltage at the load to be zero. To satisfy this, the reflected wave must be equal in magnitude but opposite in polarity to the incident wave (Vr=тИТViV_r = -V_iVrтАЛ=тИТViтАЛ). This 180┬░180┬░180┬░ phase inversion ensures that the incident and reflected waves cancel each other out at the point of short circuit.

ЁЯУМ Key Points
  • тЦ╕

    Short circuit implies ZL=0Z_L = 0ZLтАЛ=0.

  • тЦ╕

    Reflection coefficient ╬У=тИТ1\Gamma = -1╬У=тИТ1 signifies a phase change of 180┬░180┬░180┬░.

  • тЦ╕

    The incident and reflected waves interfere destructively at the load.

  • тЦ╕

    Voltage at the short circuit terminal is always zero.

тЬЕ Advantages
  • тЦ╕

    Enables determination of fault location in power lines.

  • тЦ╕

    Allows analysis of surge propagation characteristics.

тЭМ Disadvantages / Limitations
  • тЦ╕

    Results in total reflection, preventing power delivery to the load.

  • тЦ╕

    Can cause high-voltage transients if the line is not properly terminated.

ЁЯЫая╕П Applications / Uses
  • тЦ╕

    Power system protection (Fault location).

  • тЦ╕

    Time Domain Reflectometry (TDR) for cable testing.

ЁЯУД Additional Information
  • тЦ╕

    For an open-circuited line (ZL=тИЮZ_L = \inftyZLтАЛ=тИЮ), ╬У=+1\Gamma = +1╬У=+1, which corresponds to 0┬░0┬░0┬░ phase shift.

  • тЦ╕

    Option A (Zero) is incorrect as it represents a perfectly matched line (ZL=Z0Z_L = Z_0ZLтАЛ=Z0тАЛ).

ЁЯУК Diagram / Illustration
Reflection Coefficient Formula╬У = (ZтВЧ - ZтВА / ZтВЧ + ZтВА)For Short Circuit: ZтВЧ = 0╬У = (0 - ZтВА / 0 + ZтВА) = -1 = 180┬░
тЬЕ

D is correct тАФ The reflection coefficient for a short-circuited line is тИТ1-1тИТ1, which represents a phase reversal of 180┬░180┬░180┬░.

Core Concepts Used
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Traveling wave theory Boundary conditions in transmission lines Reflection coefficient
ЁЯТб EXAM TIP

Always remember: Short circuit (ZL=0Z_L=0ZLтАЛ=0) gives ╬У=тИТ1\Gamma=-1╬У=тИТ1 (180┬░180┬░180┬░), Open circuit (ZL=тИЮZ_L=\inftyZLтАЛ=тИЮ) gives ╬У=+1\Gamma=+1╬У=+1 (0┬░0┬░0┬░), and Matched line (ZL=Z0Z_L=Z_0ZLтАЛ=Z0тАЛ) gives ╬У=0\Gamma=0╬У=0.

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