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ElectricalPower System
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A rectangular voltage wave is impressed on a loss-free overhead line, with the far end of the line being short-circuited. On reaching the end of this line

A

The current wave is reflected back with positive sign, but the voltage wave with negative sign

B

The current wave is reflected back with negative sign, but the voltage wave with positive sign

C

Both the current and the voltage waves are reflected with positive sign

D

Both the current and the voltage waves are reflected with negative sign

Correct Answer

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

The current wave is reflected back with positive sign, but the voltage wave with negative sign

Quick Summary:

When a voltage wave reaches a short-circuited end of a loss-free overhead line, the voltage reflection coefficient is -1, causing the total voltage to become zero. Conversely, the current reflection coefficient is +1, causing the reflected current wave to add to the incident wave, doubling the current.

тЪЩя╕ПTETechnical SolutionConcept & Principle
ЁЯТб Explanation

When a voltage wave reaches a short-circuited end of a loss-free overhead line, the voltage reflection coefficient is -1, causing the total voltage to become zero. Conversely, the current reflection coefficient is +1, causing the reflected current wave to add to the incident wave, doubling the current.

ЁЯФв Key Formulas

╬▓v=ZLтИТZ0ZL+Z0\beta_v = \frac{Z_L - Z_0}{Z_L + Z_0}╬▓vтАЛ=ZLтАЛ+Z0тАЛZLтАЛтИТZ0тАЛтАЛ тАФ Voltage reflection coefficient

╬▓i=Z0тИТZLZ0+ZL\beta_i = \frac{Z_0 - Z_L}{Z_0 + Z_L}╬▓iтАЛ=Z0тАЛ+ZLтАЛZ0тАЛтИТZLтАЛтАЛ тАФ Current reflection coefficient

тЪЩя╕П Working Principle

The reflection coefficients for voltage (╬▓v\beta_v╬▓vтАЛ) and current (╬▓i\beta_i╬▓iтАЛ) are defined by the load impedance (ZLZ_LZLтАЛ) and surge impedance (Z0Z_0Z0тАЛ). For a short circuit, ZL=0Z_L = 0ZLтАЛ=0. Using ╬▓v=ZLтИТZ0ZL+Z0\beta_v = \frac{Z_L - Z_0}{Z_L + Z_0}╬▓vтАЛ=ZLтАЛ+Z0тАЛZLтАЛтИТZ0тАЛтАЛ, we get ╬▓v=тИТ1\beta_v = -1╬▓vтАЛ=тИТ1. Using ╬▓i=Z0тИТZLZ0+ZL\beta_i = \frac{Z_0 - Z_L}{Z_0 + Z_L}╬▓iтАЛ=Z0тАЛ+ZLтАЛZ0тАЛтИТZLтАЛтАЛ, we get ╬▓i=+1\beta_i = +1╬▓iтАЛ=+1.

ЁЯУМ Key Points
  • тЦ╕

    For a short-circuited line, ZL=0Z_L = 0ZLтАЛ=0 resulting in ╬▓v=тИТ1\beta_v = -1╬▓vтАЛ=тИТ1 and ╬▓i=+1\beta_i = +1╬▓iтАЛ=+1.

  • тЦ╕

    The reflected voltage wave cancels the incident wave at the short-circuited point to maintain zero voltage.

  • тЦ╕

    The reflected current wave reinforces the incident wave, doubling the current at the point of short circuit.

тЬЕ Advantages
  • тЦ╕

    Useful for calculating transient current spikes during line-to-ground faults.

  • тЦ╕

    Essential for understanding protection relay requirements.

тЭМ Disadvantages / Limitations
  • тЦ╕

    High current doubling can cause mechanical damage to conductors.

  • тЦ╕

    Over-voltage concerns exist if the termination was open-circuited instead.

ЁЯЫая╕П Applications / Uses
  • тЦ╕

    Protection system coordination for transmission lines.

  • тЦ╕

    Analysis of fault transients in power networks.

ЁЯУД Additional Information
  • тЦ╕

    Loss-free lines assume R=0R=0R=0 and G=0G=0G=0.

  • тЦ╕

    Option B is wrong because it swaps the signs of the reflection coefficients.

ЁЯУК Diagram / Illustration
Reflection Coefficients (ZтВЧ=0)╬▓с╡е = (0 - ZтВА / 0 + ZтВА) = -1╬▓с╡в = (ZтВА - 0 / ZтВА + 0) = +1
тЬЕ

A is correct тАФ The voltage reflection coefficient at a short circuit is -1 and the current reflection coefficient is +1.

Core Concepts Used
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Surge Impedance Reflection Coefficient Transmission Line Transients
ЁЯТб EXAM TIP

Remember: Voltage follows the polarity of the impedance mismatch, while current follows the inverse logic for short circuits (ZL=0Z_L=0ZLтАЛ=0) vs open circuits (ZL=тИЮZ_L=\inftyZLтАЛ=тИЮ).

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