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ElectricalPower System
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In case the characteristic impedance of a transmission line is equal to the load impedance

A

The system will resonate badly

B

All the energy sent will be absorbed by the load

C

All the energy sent will pass to the earth

D

All the energy will be lost in transmission line as transmission losses

Correct Answer

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

All the energy sent will be absorbed by the load

Quick Summary:

When the load impedance (ZLZ_LZLтАЛ) is exactly equal to the characteristic impedance (Z0Z_0Z0тАЛ) of a transmission line, the line is said to be 'matched'. In this state, the reflection coefficient at the load becomes zero, meaning no power is reflected back toward the source, and the entire incident power is absorbed by the load.

тЪЩя╕ПTETechnical SolutionConcept & Principle
ЁЯТб Explanation

When the load impedance (ZLZ_LZLтАЛ) is exactly equal to the characteristic impedance (Z0Z_0Z0тАЛ) of a transmission line, the line is said to be 'matched'. In this state, the reflection coefficient at the load becomes zero, meaning no power is reflected back toward the source, and the entire incident power is absorbed by the load.

ЁЯФв Key Formulas

╬У=ZLтИТZ0ZL+Z0\Gamma = \frac{Z_L - Z_0}{Z_L + Z_0}╬У=ZLтАЛ+Z0тАЛZLтАЛтИТZ0тАЛтАЛ тАФ Reflection Coefficient

SWR=1+тИг╬УтИг1тИТтИг╬УтИгSWR = \frac{1 + |\Gamma|}{1 - |\Gamma|}SWR=1тИТтИг╬УтИг1+тИг╬УтИгтАЛ тАФ Standing Wave Ratio

тЪЩя╕П Working Principle

The reflection coefficient is defined as ╬У=ZLтИТZ0ZL+Z0\Gamma = \frac{Z_L - Z_0}{Z_L + Z_0}╬У=ZLтАЛ+Z0тАЛZLтАЛтИТZ0тАЛтАЛ. When ZL=Z0Z_L = Z_0ZLтАЛ=Z0тАЛ, then ╬У=0\Gamma = 0╬У=0. Consequently, the Standing Wave Ratio (SWR) becomes 1:1, representing a traveling wave condition with no reflected waves and pure active power transfer.

ЁЯУМ Key Points
  • тЦ╕

    Maximum Power Transfer Theorem: Maximum power is delivered when load impedance equals the complex conjugate of source impedance.

  • тЦ╕

    Matched lines exhibit no standing waves, preventing potential overvoltage at the source due to reflections.

  • тЦ╕

    Return loss becomes infinite (or extremely high) when the line is perfectly matched.

  • тЦ╕

    Characteristic impedance (Z0Z_0Z0тАЛ) depends only on the physical geometry and material properties of the line.

тЬЕ Advantages
  • тЦ╕

    Elimination of reflected waves preventing standing wave interference

  • тЦ╕

    Maximum efficiency of power transfer from source to load

тЭМ Disadvantages / Limitations
  • тЦ╕

    Requires precise impedance matching components at high frequencies

  • тЦ╕

    Changes in load impedance result in immediate signal reflection

ЁЯЫая╕П Applications / Uses
  • тЦ╕

    Radio frequency (RF) transmission line matching

  • тЦ╕

    Antenna feed systems

  • тЦ╕

    High-speed digital signal integrity (PCIe, USB)

ЁЯУД Additional Information
  • тЦ╕

    When ZL=Z0Z_L = Z_0ZLтАЛ=Z0тАЛ, the transmission line appears as if it were infinitely long to the source because there is no wave reflection.

  • тЦ╕

    Option A is incorrect because resonance occurs when reflections interfere constructively; matching prevents reflections.

  • тЦ╕

    Option C is incorrect as energy is absorbed by the load, not diverted to earth.

  • тЦ╕

    Option D is incorrect because transmission losses are independent of the matching condition; they are inherent to the line's resistance.

ЁЯУК Diagram / Illustration
Reflection Coefficient (╬У)ZтВЧ - ZтВАZтВЧ + ZтВАWhen ZтВЧ = ZтВА, ╬У = 0
тЬЕ

B is correct тАФ When the line is terminated with its characteristic impedance, the reflection coefficient is zero, ensuring all incident energy is consumed by the load.

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

Always remember that Z0Z_0Z0тАЛ is purely resistive for lossless lines, but Z0Z_0Z0тАЛ is complex for lossy lines; matching in lossy lines must account for both real and reactive components.

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