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ElectricalPower System
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The velocity of propagation of electromagnetic waves on overhead line is

A

3├Ч1083 \times 10тБ╕3├Ч108 m/s

B

3├Ч1083 \times 10тБ╕3├Ч108 km/s

C

3├Ч10103 \times 10^{10}3├Ч1010 m/s

D

3├Ч1083 \times 10тБ╕3├Ч108 km/hr

Correct Answer

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

3├Ч1083 \times 10тБ╕3├Ч108 m/s

Quick Summary:

The velocity of propagation of electromagnetic waves on overhead transmission lines is approximately equal to the speed of light in free space, which is 3├Ч1083 \times 10тБ╕3├Ч108 m/s. This occurs because the electromagnetic energy travels through the surrounding air medium rather than through the metallic conductors themselves.

тЪЩя╕ПTETechnical SolutionConcept & Principle
ЁЯТб Explanation

The velocity of propagation of electromagnetic waves on overhead transmission lines is approximately equal to the speed of light in free space, which is 3├Ч1083 \times 10тБ╕3├Ч108 m/s. This occurs because the electromagnetic energy travels through the surrounding air medium rather than through the metallic conductors themselves.

ЁЯФв Key Formulas

v=1LCv = \frac{1}{\sqrt{LC}}v=LCтАЛ1тАЛ тАФ Velocity of electromagnetic wave on a transmission line

v=1╬╝0╧╡0тЙИ3├Ч108v = \frac{1}{\sqrt{\mu_0 \epsilon_0}} \approx 3 \times 10тБ╕v=╬╝0тАЛ╧╡0тАЛтАЛ1тАЛтЙИ3├Ч108 m/s тАФ Velocity in free space or air

тЪЩя╕П Working Principle

An electromagnetic wave on a transmission line is characterized by the velocity v=1LCv = \frac{1}{\sqrt{LC}}v=LCтАЛ1тАЛ, where LLL is inductance per unit length and CCC is capacitance per unit length. For an overhead line, the dielectric constant and magnetic permeability of the air are essentially those of a vacuum, leading to a velocity of propagation v=1╬╝0╧╡0=c=3├Ч108v = \frac{1}{\sqrt{\mu_0 \epsilon_0}} = c = 3 \times 10тБ╕v=╬╝0тАЛ╧╡0тАЛтАЛ1тАЛ=c=3├Ч108 m/s.

ЁЯУМ Key Points
  • тЦ╕

    Electromagnetic waves travel in the dielectric space around the conductors.

  • тЦ╕

    The velocity is inversely proportional to the square root of the line parameters (inductance and capacitance).

  • тЦ╕

    In underground cables, the velocity is lower than 3├Ч1083 \times 10тБ╕3├Ч108 m/s due to the higher permittivity of insulation materials.

тЬЕ Advantages
  • тЦ╕

    Fast transient signal propagation for protection relaying

  • тЦ╕

    Minimal time delay for communication signaling

тЭМ Disadvantages / Limitations
  • тЦ╕

    High-speed surges can cause insulation breakdown if protection is not fast enough

  • тЦ╕

    Reflection phenomenon complicates voltage analysis

ЁЯЫая╕П Applications / Uses
  • тЦ╕

    Power system transient analysis

  • тЦ╕

    Traveling wave protection schemes

  • тЦ╕

    Fault location in transmission lines

ЁЯУД Additional Information
  • тЦ╕

    The value 3├Ч1083 \times 10тБ╕3├Ч108 m/s corresponds to 300,000 km/s.

  • тЦ╕

    Option B (3├Ч10тБ╕ km/s) is incorrect as it is 10610тБ╢106 times faster than light.

  • тЦ╕

    Option C (3├Ч10┬╣тБ░ m/s) is incorrect as it is 10210┬▓102 times faster than light.

  • тЦ╕

    Option D (3├Ч10тБ╕ km/hr) is incorrect as it equals approximately 83.33 km/s.

ЁЯУК Diagram / Illustration
Propagation Velocityv = 1
LC\sqrt{LC}LCтАЛ
тЬЕ

A is correct тАФ The velocity of propagation of electromagnetic waves on overhead transmission lines is approximately the speed of light, 3├Ч1083 \times 10тБ╕3├Ч108 m/s.

Core Concepts Used
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Transmission Line Theory Electromagnetic Wave Propagation Power System Transients
ЁЯТб EXAM TIP

Remember that velocity is always lower in cables than in overhead lines because the relative permittivity ╧╡r\epsilon_r╧╡rтАЛ of insulating material is greater than 1, reducing velocity by a factor of 1/╧╡r1/\sqrt{\epsilon_r}1/╧╡rтАЛтАЛ.

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