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ElectricalPower System
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The values of A, B, C and D constants for a short transmission line are respectively

A

Z, 0, 1 and 1

B

0, 1, 1 and 1

C

1, Z, 0 and 1

D

1, 1, Z and 0

Correct Answer

Concept & PrincipleElectricalPower System
Option A

Z, 0, 1 and 1

Quick Summary: For a short transmission line, the series impedance is represented by Z and the shunt admittance is assumed to be negligible. The ABCD parameters (or transmission parameters) relate the sending end voltage and current to the receiving end values via the matrix equation [V_s, I_s]^T = [[A, B], [C, D]] [V_r, I_r]^T.

ЁЯТб Explanation

For a short transmission line, the series impedance is represented by Z and the shunt admittance is assumed to be negligible. The ABCD parameters (or transmission parameters) relate the sending end voltage and current to the receiving end values via the matrix equation [VsV_{s}VsтАЛ, IsI_{s}IsтАЛ]^T = [[A, B], [C, D]] [VrV_{r}VrтАЛ, IrI_{r}IrтАЛ]^T.

ЁЯФв Key Formulas

Vs=AVr+BIrV_s = A V_r + B I_rVsтАЛ=AVrтАЛ+BIrтАЛ тАФ Sending end voltage equation

Is=CVr+DIrI_s = C V_r + D I_rIsтАЛ=CVrтАЛ+DIrтАЛ тАФ Sending end current equation

A=D=1,B=Z,C=0A = D = 1, B = Z, C = 0A=D=1,B=Z,C=0 тАФ ABCD constants for short line

тЪЩя╕П Working Principle

In a short transmission line, the line length is typically less than 80 km. Due to the short length, the shunt capacitance is so small that it is neglected, leading to an admittance Y = 0. Applying Kirchhoff's Voltage and Current Laws at the receiving end yields VsV_{s}VsтАЛ = VrV_{r}VrтАЛ + IrI_{r}IrтАЛ Z and IsI_{s}IsтАЛ = IrI_{r}IrтАЛ, which corresponds to the ABCD matrix [[1, Z], [0, 1]].

ЁЯУМ Key Points
  • тЦ╕

    Short transmission lines are defined by lengths < 80 km or operating voltages below 20 kV.

  • тЦ╕

    Shunt admittance (Y) is neglected, setting C = 0.

  • тЦ╕

    The parameter A is equal to D due to the reciprocal nature of the transmission line.

  • тЦ╕

    The parameter B represents the series impedance Z of the line.

тЬЕ Advantages
  • тЦ╕

    Simplifies power flow calculations for distribution networks.

  • тЦ╕

    Provides a highly accurate model for short-distance local power delivery.

тЭМ Disadvantages / Limitations
  • тЦ╕

    Inaccurate for long transmission lines where shunt capacitance cannot be ignored.

  • тЦ╕

    Does not account for Ferranti effect or line charging currents.

ЁЯЫая╕П Applications / Uses
  • тЦ╕

    Distribution networks.

  • тЦ╕

    Local sub-transmission lines.

ЁЯУД Additional Information
  • тЦ╕

    For short lines, the condition ADтИТBC=1AD - BC = 1ADтИТBC=1 is satisfied as (1)(1)тИТ(Z)(0)=1(1)(1) - (Z)(0) = 1(1)(1)тИТ(Z)(0)=1.

  • тЦ╕

    Option A is incorrect because Z should be in the B position, not A.

  • тЦ╕

    Option D is incorrect as it represents an inverse or invalid parameter configuration.

ЁЯУК Diagram / Illustration
Short Transmission Line MatrixVтВЫ=1Z01[Vс╡г, Iс╡г]с╡А
тЬЕ

C is correct тАФ For a short transmission line, the ABCD constants are A=1, B=Z, C=0, and D=1.

Core Concepts Used
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ABCD Parameters Transmission Line Modeling Kirchhoff's Laws
ЁЯТб EXAM TIP

Remember that for all passive, linear, two-port networks, the condition ADтИТBC=1AD - BC = 1ADтИТBC=1 always holds; verify this in exams to eliminate wrong options.

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