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ElectricalPower System
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If the receiving-end voltage and current are numerically equal to the corresponding sending-end values, that is, |Vs| = |Vr| and |Is| = |Ir|, then such a line is called

A

An infinite line

B

A natural line

C

A tuned line

D

A loss-less line

Correct Answer

Concept & PrincipleElectricalPower System
Option A

An infinite line

Quick Summary: An infinite line is a theoretical transmission line where the receiving-end voltage and current magnitudes are identical to the sending-end values because the line is terminated by its characteristic impedance. In this condition, the input impedance of the line equals its characteristic impedance ($Z_{in} = Z_0$), resulting in no reflections.

ЁЯТб Explanation

An infinite line is a theoretical transmission line where the receiving-end voltage and current magnitudes are identical to the sending-end values because the line is terminated by its characteristic impedance. In this condition, the input impedance of the line equals its characteristic impedance (Zin=Z0Z_{in} = Z_0ZinтАЛ=Z0тАЛ), resulting in no reflections.

ЁЯФв Key Formulas

Zin=Z0ZR+Z0tanhтБб(╬│l)Z0+ZRtanhтБб(╬│l)Z_{in} = Z_0 \frac{Z_R + Z_0 \tanh(\gamma l)}{Z_0 + Z_R \tanh(\gamma l)}ZinтАЛ=Z0тАЛZ0тАЛ+ZRтАЛtanh(╬│l)ZRтАЛ+Z0тАЛtanh(╬│l)тАЛ тАФ General input impedance formula

Zin=Z0Z_{in} = Z_0ZinтАЛ=Z0тАЛ тАФ Condition for an infinite line where ZR=Z0Z_R = Z_0ZRтАЛ=Z0тАЛ

тЪЩя╕П Working Principle

When a transmission line is terminated with a load impedance equal to its characteristic impedance (ZR=Z0Z_R = Z_0ZRтАЛ=Z0тАЛ), all incident power is absorbed by the load. Consequently, the voltage and current profiles are uniform throughout the line, behaving as if the line were infinitely long without any reflected waves returning to the source.

ЁЯУМ Key Points
  • тЦ╕

    Input impedance is independent of line length lll.

  • тЦ╕

    Reflection coefficient ╬У=0\Gamma = 0╬У=0 at the load.

  • тЦ╕

    Uniform voltage and current magnitude along the line.

  • тЦ╕

    The line appears as a pure resistance Z0Z_0Z0тАЛ to the source.

тЬЕ Advantages
  • тЦ╕

    No reflected waves exist on the line.

  • тЦ╕

    Maximum power transfer condition is inherently satisfied.

тЭМ Disadvantages / Limitations
  • тЦ╕

    Theoretical construct; physically infinite lines do not exist.

  • тЦ╕

    Practical limitations due to line losses (alphaneq0\\alpha \\neq 0alphaneq0) making perfect impedance matching difficult.

ЁЯЫая╕П Applications / Uses
  • тЦ╕

    Foundation for analyzing wave propagation in transmission lines.

  • тЦ╕

    Impedance matching techniques in high-frequency RF systems.

ЁЯУД Additional Information
  • тЦ╕

    A 'natural line' (Option B) usually refers to a line operating at surge impedance loading (SIL).

  • тЦ╕

    A 'tuned line' (Option C) refers to a line with length lambda/2\\lambda/2lambda/2 or lambda/4\\lambda/4lambda/4 where input impedance equals load impedance or its inverse.

  • тЦ╕

    A 'loss-less line' (Option D) has R=0R=0R=0 and G=0G=0G=0 but does not necessarily imply Vs=VrV_s = V_rVsтАЛ=VrтАЛ.

ЁЯУК Diagram / Illustration
Infinite Line ConditionZс╡втВЩ = VтВЫ / IтВЫZтВА = Vс╡г / Iс╡гSourceLoad
тЬЕ

A is correct тАФ An infinite line is defined by the condition where the line is terminated by its characteristic impedance, resulting in no reflection and identical magnitudes at both ends.

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

Always remember that for an infinite line, the input impedance is purely equal to the characteristic impedance Z0Z_0Z0тАЛ, regardless of the electrical length of the line.

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