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ElectricalPower System
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The propagation constant of a transmission line is 0.15├Ч10тАУ┬│ + j1.5├Ч10тАУ┬│. The wavelength of the traveling wave is

A

15├Ч10тИТ32╧А\frac{15 \times 10^{-3}}{2\pi}2╧А15├Ч10тИТ3тАЛ

B

2╧А1.5├Ч10тИТ3\frac{2\pi}{1.5 \times 10^{-3}}1.5├Ч10тИТ32╧АтАЛ

C

15├Ч10тИТ3╧А\frac{15 \times 10^{-3}}{\pi}╧А15├Ч10тИТ3тАЛ

D

╧А15├Ч10тИТ3\frac{\pi}{15 \times 10^{-3}}15├Ч10тИТ3╧АтАЛ

Correct Answer

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

2╧А1.5├Ч10тИТ3\frac{2\pi}{1.5 \times 10^{-3}}1.5├Ч10тИТ32╧АтАЛ

Quick Summary:

The propagation constant of a transmission line is defined as ╬│=╬▒+j╬▓\gamma = \alpha + j\beta╬│=╬▒+j╬▓, where ╬▒\alpha╬▒ is the attenuation constant and ╬▓\beta╬▓ is the phase constant. The wavelength ╬╗\lambda╬╗ of the traveling wave is related to the phase constant ╬▓\beta╬▓ by the expression ╬╗=2╧А╬▓\lambda = \frac{2\pi}{\beta}╬╗=╬▓2╧АтАЛ.

тЪЩя╕ПTETechnical SolutionConcept & Principle
ЁЯТб Explanation

The propagation constant of a transmission line is defined as ╬│=╬▒+j╬▓\gamma = \alpha + j\beta╬│=╬▒+j╬▓, where ╬▒\alpha╬▒ is the attenuation constant and ╬▓\beta╬▓ is the phase constant. The wavelength ╬╗\lambda╬╗ of the traveling wave is related to the phase constant ╬▓\beta╬▓ by the expression ╬╗=2╧А╬▓\lambda = \frac{2\pi}{\beta}╬╗=╬▓2╧АтАЛ.

ЁЯФв Key Formulas

╬│=╬▒+j╬▓\gamma = \alpha + j\beta╬│=╬▒+j╬▓ тАФ Propagation constant definition

╬╗=2╧А╬▓\lambda = \frac{2\pi}{\beta}╬╗=╬▓2╧АтАЛ тАФ Relationship between wavelength and phase constant

тЪЩя╕П Working Principle

As an electromagnetic wave propagates down a transmission line, it undergoes a phase shift determined by the phase constant ╬▓\beta╬▓. The distance required for the wave to complete one full cycle (a phase shift of 2╧А2\pi2╧А radians) is defined as the wavelength ╬╗\lambda╬╗. Since ╬▓\beta╬▓ represents the phase shift per unit length (radians/meter), ╬╗\lambda╬╗ is simply the inverse proportion of ╬▓\beta╬▓.

ЁЯУМ Key Points
  • тЦ╕

    The propagation constant is a complex quantity where the imaginary part ╬▓\beta╬▓ dictates the wave's phase velocity.

  • тЦ╕

    The units of ╬▓\beta╬▓ are radians per meter (rad/m) and ╬▒\alpha╬▒ are nepers per meter (Np/m).

  • тЦ╕

    Wavelength is inversely proportional to the phase constant: higher frequency signals generally correspond to higher ╬▓\beta╬▓ values and shorter wavelengths.

тЬЕ Advantages
  • тЦ╕

    Provides a simple mathematical relation for wave analysis

  • тЦ╕

    Essential for calculating line impedance matching

тЭМ Disadvantages / Limitations
  • тЦ╕

    Assumes a linear, time-invariant transmission line

  • тЦ╕

    Does not account for non-uniform line geometry

ЁЯЫая╕П Applications / Uses
  • тЦ╕

    Designing impedance matching networks

  • тЦ╕

    Determining signal propagation delays in power and communication lines

ЁЯУД Additional Information
  • тЦ╕

    Given ╬│=0.15├Ч10тИТ3+j(1.5├Ч10тИТ3)\gamma = 0.15 \times 10^{-3} + j(1.5 \times 10^{-3})╬│=0.15├Ч10тИТ3+j(1.5├Ч10тИТ3), the imaginary part ╬▓=1.5├Ч10тИТ3\beta = 1.5 \times 10^{-3}╬▓=1.5├Ч10тИТ3.

  • тЦ╕

    Substituting ╬▓\beta╬▓ into the formula ╬╗=2╧А╬▓\lambda = \frac{2\pi}{\beta}╬╗=╬▓2╧АтАЛ yields 2╧А1.5├Ч10тИТ3\frac{2\pi}{1.5 \times 10^{-3}}1.5├Ч10тИТ32╧АтАЛ.

ЁЯУК Diagram / Illustration
Wavelength Formula╬╗ = 2╧А╬▓
тЬЕ

B is correct тАФ The wavelength is defined by ╬╗=2╧А╬▓\lambda = \frac{2\pi}{\beta}╬╗=╬▓2╧АтАЛ, where ╬▓\beta╬▓ is the imaginary part of the propagation constant.

Core Concepts Used
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Transmission Line Theory Propagation Constant Wave Physics
ЁЯТб EXAM TIP

Always ensure you extract the imaginary part (╬▓\beta╬▓) for phase calculations, as the real part (╬▒\alpha╬▒) only affects signal amplitude/attenuation.

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