Examoogle
ExamsTest SeriesCBATRank CheckPrevious Year PapersPassBook StoreMy BooksAI Tutor
ЁЯЫТ0
рдЕA
Examoogle

India's most trusted platform for competitive exam PDF books. Expert-authored, watermark-protected, instant access.

Exams & Practice
All Exams & SyllabusMock Test SeriesPrevious Year PapersPractice Questions (MCQs)Recruitment Notifications
Quick Links
Examoogle AI TutorExam NewsBook StoreMy BooksLogin / Sign Up
Support
About UsRefund PolicyPrivacy PolicyTerms of UseContact Us
┬й 2026 Examoogle. India's #1 competitive exam AI tutor.
ЁЯФТ SSL SecuredЁЯУ▒ UPI AcceptedЁЯз╛ GST Invoice
Examoogle

Join 60,000+ competitive exam aspirants

or with email
By continuing, you agree to ourTerms of Service&Privacy Policy
Your Cart
SubtotalтВ╣0
TotalтВ╣0
Examoogle тАв User тАв info@examoogle.com тАв EE-2024-8821
Chapter 1 of 12 тАв Page 1 of 248ЁЯФТ Protected PDF тАв Watermarked
Back to Practice Questions
ElectricalPower System
PrevNext

Under no load conditions the current in a transmission line is because of

A

Capacitance effect

B

Corona effect

C

Proximity effect

D

Back flow from earth

Correct Answer

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

Capacitance effect

Quick Summary:

Under no-load conditions, a transmission line behaves like a large capacitor due to the potential difference between conductors separated by air (dielectric). This distributed shunt capacitance draws a leading charging current from the source, even when no active power is being delivered to a load.

тЪЩя╕ПTETechnical SolutionConcept & Principle
ЁЯТб Explanation

Under no-load conditions, a transmission line behaves like a large capacitor due to the potential difference between conductors separated by air (dielectric). This distributed shunt capacitance draws a leading charging current from the source, even when no active power is being delivered to a load.

ЁЯФв Key Formulas

Ich=VphтЛЕ2╧АfCI_{ch} = V_{ph} \cdot 2\pi f CIchтАЛ=VphтАЛтЛЕ2╧АfC тАФ Charging current in a transmission line

C=2╧А╧╡0lnтБб(D/r)C = \frac{2\pi \epsilon_0}{\ln(D/r)}C=ln(D/r)2╧А╧╡0тАЛтАЛ тАФ Capacitance per unit length of a two-wire line

тЪЩя╕П Working Principle

The conductors of a transmission line form the plates of a capacitor, and the air between them acts as the dielectric medium. Since the line is energized by an AC voltage, the charging current flows through these shunt capacitors. This current is given by Ich=VphтЛЕ╧ЙCI_{ch} = V_{ph} \cdot \omega CIchтАЛ=VphтАЛтЛЕ╧ЙC, leading to the Ferranti effect, where the receiving end voltage can become higher than the sending end voltage at no-load.

ЁЯУМ Key Points
  • тЦ╕

    Charging current is capacitive and leads the voltage by 90 degrees.

  • тЦ╕

    This effect is more pronounced in long transmission lines at high voltages.

  • тЦ╕

    The Ferranti effect is a direct consequence of this no-load capacitive charging current.

  • тЦ╕

    Shunt reactors are often used to compensate for this effect at light loads.

тЬЕ Advantages
  • тЦ╕

    Helps in maintaining voltage profile in long lines

  • тЦ╕

    Provides reactive power support

тЭМ Disadvantages / Limitations
  • тЦ╕

    Causes rise in receiving end voltage (Ferranti effect)

  • тЦ╕

    Can lead to insulation stress during overvoltage conditions

ЁЯЫая╕П Applications / Uses
  • тЦ╕

    EHV (Extra High Voltage) transmission line planning

  • тЦ╕

    Reactive power compensation studies

ЁЯУД Additional Information
  • тЦ╕

    Corona effect occurs only when the electric field intensity exceeds the dielectric strength of air (approx 30 kV/cm).

  • тЦ╕

    Proximity effect is due to the non-uniform distribution of current in conductors due to magnetic fields of nearby conductors, significant only under load.

  • тЦ╕

    Back flow from earth is not a standard term for no-load current mechanisms.

ЁЯУК Diagram / Illustration
No-Load Charging Current
Ich=VphтЛЕ2╧АfCI_{ch} = V_{ph} \cdot 2\pi f CIchтАЛ=VphтАЛтЛЕ2╧АfC
Source VoltageLine C
Charging Current flows due to CCC
тЬЕ

A is correct тАФ The no-load current is primarily the charging current required to charge the shunt capacitance of the transmission line.

Core Concepts Used
Click any tag to open in AI Tutor
Transmission Line Capacitance Charging Current Ferranti Effect
ЁЯТб EXAM TIP

Always remember that charging current is proportional to the line length and voltage; hence, it becomes critical in EHV/UHV lines (400kV and above).

Related Questions

ElectricalPower System
The specified quantities of Generation bus is
ElectricalPower System
When an alternator connected to the bus-bar is shut down the bus-bar voltage will
ElectricalPower System
The current drawn by the line due to corona losses is _______
ElectricalPower System
The specified quantities of load bus are
ElectricalPower System
The advantages of high transmission voltage are ______

Discussion (0)

Loading discussion...
PrevNext