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ElectricalPower System
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The performance equations of any branch тАШiтАЩ in impedance form will be'

A

Vi+ei=Zi├ЧIiV_i + e_i = Z_i \times I_iViтАЛ+eiтАЛ=ZiтАЛ├ЧIiтАЛ

B

Vi=Zi├ЧIiV_i = Z_i \times I_iViтАЛ=ZiтАЛ├ЧIiтАЛ

C

ViтИТei=ZiV_i - e_i = Z_iViтАЛтИТeiтАЛ=ZiтАЛ

D

ViтИТei=Zi├ЧIiV_i - e_i = Z_i \times I_iViтАЛтИТeiтАЛ=ZiтАЛ├ЧIiтАЛ

Correct Answer

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

Vi+ei=Zi├ЧIiV_i + e_i = Z_i \times I_iViтАЛ+eiтАЛ=ZiтАЛ├ЧIiтАЛ

Quick Summary:

In power system network analysis, any branch 'i' of a network consists of a series impedance ZiZ_iZiтАЛ and an internal source eie_ieiтАЛ. The branch performance equation describes the relationship between the terminal voltage ViV_iViтАЛ, internal emf eie_ieiтАЛ, and the current IiI_iIiтАЛ flowing through the branch.

тЪЩя╕ПTETechnical SolutionConcept & Principle
ЁЯТб Explanation

In power system network analysis, any branch 'i' of a network consists of a series impedance ZiZ_iZiтАЛ and an internal source eie_ieiтАЛ. The branch performance equation describes the relationship between the terminal voltage ViV_iViтАЛ, internal emf eie_ieiтАЛ, and the current IiI_iIiтАЛ flowing through the branch.

ЁЯФв Key Formulas

Vi+ei=Zi├ЧIiV_i + e_i = Z_i \times I_iViтАЛ+eiтАЛ=ZiтАЛ├ЧIiтАЛ тАФ Branch performance equation in impedance form

Ii=Yi(Vi+ei)I_i = Y_i(V_i + e_i)IiтАЛ=YiтАЛ(ViтАЛ+eiтАЛ) тАФ Admittance form of the branch equation

тЪЩя╕П Working Principle

According to Kirchhoff's Voltage Law applied to a branch, the terminal voltage ViV_iViтАЛ plus the internal source emf eie_ieiтАЛ must balance the voltage drop across the branch impedance ZiIiZ_i I_iZiтАЛIiтАЛ. The branch impedance ZiZ_iZiтАЛ accounts for the resistive and reactive properties of the line or component, while eie_ieiтАЛ represents any active voltage source within that branch.

ЁЯУМ Key Points
  • тЦ╕

    The equation Vi+ei=ZiIiV_i + e_i = Z_i I_iViтАЛ+eiтАЛ=ZiтАЛIiтАЛ assumes the convention where eie_ieiтАЛ is a series voltage source.

  • тЦ╕

    Branch performance equations are fundamental for building the Z-bus (impedance matrix) for power flow studies.

  • тЦ╕

    In the absence of an internal source, eie_ieiтАЛ becomes zero, simplifying the expression to Vi=ZiIiV_i = Z_i I_iViтАЛ=ZiтАЛIiтАЛ.

тЬЕ Advantages
  • тЦ╕

    Allows systematic formation of bus impedance matrices.

  • тЦ╕

    Easily accounts for series compensation and internal line voltage sources.

тЭМ Disadvantages / Limitations
  • тЦ╕

    Does not account for shunt elements directly without modification.

  • тЦ╕

    Requires complex arithmetic as Z is a complex quantity (R + jX).

ЁЯЫая╕П Applications / Uses
  • тЦ╕

    Power system load flow analysis.

  • тЦ╕

    Short circuit calculations and fault analysis.

ЁЯУД Additional Information
  • тЦ╕

    Option B (Vi=Zi├ЧIiV_i = Z_i \times I_iViтАЛ=ZiтАЛ├ЧIiтАЛ) is only true for passive branches without internal EMF sources.

  • тЦ╕

    Options C and D are mathematically incorrect representations of the KVL loop equation for the specified branch model.

ЁЯУК Diagram / Illustration
Branch Performance EquationVс╡в + eс╡в = Zс╡в ├Ч Iс╡вWhere V = Terminal Voltage, e = Source EMF, Z = Impedance, I = Branch Current
тЬЕ

A is correct тАФ The performance equation Vi+ei=Zi├ЧIiV_i + e_i = Z_i \times I_iViтАЛ+eiтАЛ=ZiтАЛ├ЧIiтАЛ correctly satisfies Kirchhoff's Voltage Law for a branch containing a series impedance and a voltage source.

Core Concepts Used
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Kirchhoff's Voltage Law Branch Impedance Model Network Topology
ЁЯТб EXAM TIP

Remember that in admittance form (Y=ZтИТ1Y = Z^{-1}Y=ZтИТ1), the equation becomes Ii=Yi(Vi+ei)I_i = Y_i(V_i + e_i)IiтАЛ=YiтАЛ(ViтАЛ+eiтАЛ), which is frequently tested in nodal analysis.

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