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ElectricalPower System
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A long overhead transmission line is terminated by its characteristic impedance. Under this operating condition, the ratio of the voltage to the current at different points along the line will

A

Progressively increase from the sending-end to the receiving-end

B

Progressively increase from the receiving-end to the sending-end

C

Remain the same at the two ends, but is higher between the two end being maximum at the centre of the line

D

Remain the same at all points

Correct Answer

Concept & PrincipleElectricalPower System
Option D

Remain the same at all points

Quick Summary: When a transmission line is terminated by its characteristic impedance $Z_0$, the line is said to be 'matched'. Under this condition, there is no reflected wave, and the ratio of voltage to current is constant at every point along the line, equal to $Z_0$.

ЁЯТб Explanation

When a transmission line is terminated by its characteristic impedance Z0Z_0Z0тАЛ, the line is said to be 'matched'. Under this condition, there is no reflected wave, and the ratio of voltage to current is constant at every point along the line, equal to Z0Z_0Z0тАЛ.

ЁЯФв Key Formulas

Z0=R+j╧ЙLG+j╧ЙCZ_0 = \sqrt{\frac{R + j\omega L}{G + j\omega C}}Z0тАЛ=G+j╧ЙCR+j╧ЙLтАЛтАЛ тАФ characteristic impedance of a transmission line

V(x)I(x)=Z0\frac{V(x)}{I(x)} = Z_0I(x)V(x)тАЛ=Z0тАЛ тАФ constant ratio when terminated by Z0Z_0Z0тАЛ

тЪЩя╕П Working Principle

The voltage and current at any point xxx on a lossy transmission line are given by V(x)=V+eтИТ╬│x+VтИТe╬│xV(x) = V^+ e^{-\gamma x} + V^- e^{\gamma x}V(x)=V+eтИТ╬│x+VтИТe╬│x and I(x)=V+Z0eтИТ╬│xтИТVтИТZ0e╬│xI(x) = \frac{V^+}{Z_0} e^{-\gamma x} - \frac{V^-}{Z_0} e^{\gamma x}I(x)=Z0тАЛV+тАЛeтИТ╬│xтИТZ0тАЛVтИТтАЛe╬│x. If the line is terminated by ZL=Z0Z_L = Z_0ZLтАЛ=Z0тАЛ, the reflection coefficient ╬У=ZLтИТZ0ZL+Z0\Gamma = \frac{Z_L - Z_0}{Z_L + Z_0}╬У=ZLтАЛ+Z0тАЛZLтАЛтИТZ0тАЛтАЛ becomes zero, meaning VтИТ=0V^- = 0VтИТ=0. Consequently, the ratio V(x)I(x)=Z0\frac{V(x)}{I(x)} = Z_0I(x)V(x)тАЛ=Z0тАЛ remains constant regardless of the position xxx.

ЁЯУМ Key Points
  • тЦ╕

    Matched termination prevents reflections on the line.

  • тЦ╕

    A matched line behaves as if it were infinitely long.

  • тЦ╕

    The input impedance of a matched line is independent of the line length.

  • тЦ╕

    Maximum power transfer occurs when source impedance equals characteristic impedance.

тЬЕ Advantages
  • тЦ╕

    Elimination of standing waves

  • тЦ╕

    Prevention of signal reflection/distortion

тЭМ Disadvantages / Limitations
  • тЦ╕

    Not always possible due to varying load conditions

  • тЦ╕

    Requires impedance matching networks for non-ideal loads

ЁЯЫая╕П Applications / Uses
  • тЦ╕

    RF transmission lines

  • тЦ╕

    Telecommunication cabling

  • тЦ╕

    Pulse power systems

ЁЯУД Additional Information
  • тЦ╕

    If ZLтЙаZ0Z_L \neq Z_0ZLтАЛюАа=Z0тАЛ, standing waves are formed, and the ratio V/IV/IV/I varies as a function of the distance from the load.

  • тЦ╕

    Option D is the correct physical interpretation of a matched transmission line.

ЁЯУК Diagram / Illustration
Characteristic Impedance RatioV(x)I(x)= ZтВА (Constant)
тЬЕ

D is correct тАФ Because the line is terminated by its characteristic impedance, no reflection occurs, ensuring the voltage-to-current ratio remains constant at Z0Z_0Z0тАЛ throughout the line length.

Core Concepts Used
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Characteristic Impedance Reflection Coefficient Transmission Line Matching
ЁЯТб EXAM TIP

Always remember that a line terminated in Z0Z_0Z0тАЛ is 'electrically invisible' to the source; it simply looks like a fixed resistor Z0Z_0Z0тАЛ regardless of the line length.

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