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ElectricalPower System
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In overhead line with surge impedance of 400 ╬й is connected to a transformer by a short length of cable of surge impedance of 100 ╬й. If a rectangular wave of 40 kV travels along the line towards the cable than the voltage of the wave traveling from the junction of overhead line through the cable toward the transformer will be

A

16 kV

B

24 kV

C

32 kV

D

36 kV

Correct Answer

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

16 kV

Quick Summary:

When a traveling wave encounters a change in surge impedance (junction), a portion of the wave is transmitted and a portion is reflected. The voltage of the transmitted wave (VtV_tVtтАЛ) is determined by the refraction coefficient of the junction between the overhead line and the cable.

тЪЩя╕ПTETechnical SolutionConcept & Principle
ЁЯТб Explanation

When a traveling wave encounters a change in surge impedance (junction), a portion of the wave is transmitted and a portion is reflected. The voltage of the transmitted wave (VtV_tVtтАЛ) is determined by the refraction coefficient of the junction between the overhead line and the cable.

ЁЯФв Key Formulas

Vt=2Z2Z1+Z2├ЧViV_t = \frac{2Z_2}{Z_1 + Z_2} \times V_iVtтАЛ=Z1тАЛ+Z2тАЛ2Z2тАЛтАЛ├ЧViтАЛ тАФ Transmitted voltage at junction

Vr=Z2тИТZ1Z2+Z1├ЧViV_r = \frac{Z_2 - Z_1}{Z_2 + Z_1} \times V_iVrтАЛ=Z2тАЛ+Z1тАЛZ2тАЛтИТZ1тАЛтАЛ├ЧViтАЛ тАФ Reflected voltage at junction

тЪЩя╕П Working Principle

The refraction coefficient (╬▒\alpha╬▒) at the junction is calculated as ╬▒=2Z2Z1+Z2\alpha = \frac{2Z_2}{Z_1 + Z_2}╬▒=Z1тАЛ+Z2тАЛ2Z2тАЛтАЛ, where Z1=400┬а╬йZ_1 = 400 \ \OmegaZ1тАЛ=400┬а╬й (overhead line) and Z2=100┬а╬йZ_2 = 100 \ \OmegaZ2тАЛ=100┬а╬й (cable). The transmitted voltage is Vt=╬▒├ЧVincidentV_t = \alpha \times V_{incident}VtтАЛ=╬▒├ЧVincidentтАЛ. Substituting the values gives Vt=(2├Ч100400+100)├Ч40┬аkV=(200500)├Ч40┬аkV=0.4├Ч40┬аkV=16┬аkVV_t = (\frac{2 \times 100}{400 + 100}) \times 40 \text{ kV} = (\frac{200}{500}) \times 40 \text{ kV} = 0.4 \times 40 \text{ kV} = 16 \text{ kV}VtтАЛ=(400+1002├Ч100тАЛ)├Ч40┬аkV=(500200тАЛ)├Ч40┬аkV=0.4├Ч40┬аkV=16┬аkV.

ЁЯУМ Key Points
  • тЦ╕

    Surge impedance discontinuity causes wave reflection and refraction.

  • тЦ╕

    Transmission of voltage waves is governed by the refraction coefficient.

  • тЦ╕

    Since Z2<Z1Z_2 < Z_1Z2тАЛ<Z1тАЛ, the transmitted voltage wave magnitude is lower than the incident wave magnitude.

  • тЦ╕

    The sum of reflected voltage and incident voltage equals the transmitted voltage at the junction.

тЬЕ Advantages
  • тЦ╕

    Predictable behavior for insulation coordination.

  • тЦ╕

    Allows calculation of stress on equipment connected to transmission lines.

тЭМ Disadvantages / Limitations
  • тЦ╕

    Reflected waves can cause voltage doubling if the cable end is open.

  • тЦ╕

    Complex analysis required for multiple junctions.

ЁЯЫая╕П Applications / Uses
  • тЦ╕

    Protection of transformers using lightning arresters.

  • тЦ╕

    Insulation coordination in power grids.

ЁЯУД Additional Information
  • тЦ╕

    Here Z1=400┬а╬йZ_1 = 400 \ \OmegaZ1тАЛ=400┬а╬й and Z2=100┬а╬йZ_2 = 100 \ \OmegaZ2тАЛ=100┬а╬й.

  • тЦ╕

    Option B (24 kV) would result if one erroneously calculated the reflection instead of transmission, or used incorrect impedance values.

ЁЯУК Diagram / Illustration
Refraction Coefficient Calculation╬▒ = (2ZтВВ / ZтВБ + ZтВВ)╬▒ = (2 ├Ч 100 / 400 + 100) = 0.4
тЬЕ

A is correct тАФ The transmitted voltage is calculated using the refraction coefficient, resulting in 16 kV.

Core Concepts Used
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Surge Impedance Traveling Wave Theory Reflection and Refraction Coefficients
ЁЯТб EXAM TIP

Remember that if Z2<Z1Z_2 < Z_1Z2тАЛ<Z1тАЛ, the transmitted voltage is always less than the incident voltage; if Z2>Z1Z_2 > Z_1Z2тАЛ>Z1тАЛ, the transmitted voltage is greater than the incident voltage.

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