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
ElectricalElectromagnetics Field Theory
PrevNext

For any conductor, the Maxwell's second equation is

A

Curl(H) = Jc

B

Curl(E) = Jc

C

Curl(E) = Jd

D

Curl(H) = Jd

Correct Answer

тЪЩя╕П TE тАв Technical Concept & PrincipleElectricalElectromagnetics Field Theory
Option A

Curl(H) = Jc

Quick Summary:

Maxwell's second equation (derived from Ampere's Circuital Law) states that the curl of the magnetic field intensity vector HтГЧ\vec{H}H is equal to the current density JтГЧ\vec{J}J. For a conductive medium, the conduction current density JтГЧc\vec{J}_cJcтАЛ is the dominant term.

тЪЩя╕ПTETechnical SolutionConcept & Principle
ЁЯТб Explanation

Maxwell's second equation (derived from Ampere's Circuital Law) states that the curl of the magnetic field intensity vector HтГЧ\vec{H}H is equal to the current density JтГЧ\vec{J}J. For a conductive medium, the conduction current density JтГЧc\vec{J}_cJcтАЛ is the dominant term.

ЁЯФв Key Formulas

тИЗ├ЧHтГЧ=JтГЧc+тИВDтГЧтИВt\nabla \times \vec{H} = \vec{J}_c + \frac{\partial\vec{D}}{\partial t}тИЗ├ЧH=JcтАЛ+тИВtтИВDтАЛ тАФ Generalized Ampere's Law

тИЗ├ЧHтГЧ=JтГЧc\nabla \times \vec{H} = \vec{J}_cтИЗ├ЧH=JcтАЛ тАФ Form for conductive media

тЪЩя╕П Working Principle

In a perfect conductor or good conductor, the displacement current density JтГЧd\vec{J}_dJdтАЛ (given by тИВDтГЧтИВt\frac{\partial\vec{D}}{\partial t}тИВtтИВDтАЛ) is negligible compared to the conduction current density JтГЧc=╧ГEтГЧ\vec{J}_c = \sigma\vec{E}JcтАЛ=╧ГE. Thus, the differential form of Ampere's Law simplifies from тИЗ├ЧHтГЧ=JтГЧc+тИВDтГЧтИВt\nabla \times \vec{H} = \vec{J}_c + \frac{\partial\vec{D}}{\partial t}тИЗ├ЧH=JcтАЛ+тИВtтИВDтАЛ to тИЗ├ЧHтГЧ=JтГЧc\nabla \times \vec{H} = \vec{J}_cтИЗ├ЧH=JcтАЛ.

ЁЯУМ Key Points
  • тЦ╕

    Maxwell's equations are the foundation of classical electromagnetism.

  • тЦ╕

    The second equation relates the magnetic field to the current density.

  • тЦ╕

    For conductors, ╧Г\sigma╧Г is large, making JтГЧc\vec{J}_cJcтАЛ the dominant component.

тЬЕ Advantages
  • тЦ╕

    Provides a clear relationship between magnetic fields and source currents.

  • тЦ╕

    Allows for the simplification of field problems in metallic structures.

тЭМ Disadvantages / Limitations
  • тЦ╕

    Only holds true for non-time-varying displacement fields in conductors.

  • тЦ╕

    Does not account for non-ohmic conduction.

ЁЯЫая╕П Applications / Uses
  • тЦ╕

    Designing transmission lines and cables.

  • тЦ╕

    Analyzing electromagnetic shielding in conductors.

ЁЯУД Additional Information
  • тЦ╕

    In vacuum or dielectrics, JтГЧc=0\vec{J}_c = 0JcтАЛ=0, meaning тИЗ├ЧHтГЧ=тИВDтГЧтИВt\nabla \times \vec{H} = \frac{\partial\vec{D}}{\partial t}тИЗ├ЧH=тИВtтИВDтАЛ.

  • тЦ╕

    Option B and C are incorrect because the curl of the Electric Field intensity EтГЧ\vec{E}E describes Faraday's Law, not Ampere's Law.

ЁЯУК Diagram / Illustration
Maxwell's Second Equation (Conductor)
тИЗ├ЧHтГЧ\nabla \times \vec{H}тИЗ├ЧH
JтГЧc\vec{J}_cJcтАЛ
тЬЕ

A is correct тАФ Maxwell's second equation for a conductor is expressed as тИЗ├ЧHтГЧ=JтГЧc\nabla \times \vec{H} = \vec{J}_cтИЗ├ЧH=JcтАЛ.

Core Concepts Used
Click any tag to open in AI Tutor
Ampere's Circuital Law Conduction Current Density Maxwell's Equations
ЁЯТб EXAM TIP

Remember that Maxwell's 1st is Gauss's Law (ablaтЛЕDтГЧ=╧Б abla \cdot \vec{D} = \rhoablaтЛЕD=╧Б), 2nd is Ampere's Law (тИЗ├ЧHтГЧ=JтГЧ\nabla \times \vec{H} = \vec{J}тИЗ├ЧH=J), 3rd is Gauss's Law for Magnetism (тИЗтЛЕBтГЧ=0\nabla \cdot \vec{B} = 0тИЗтЛЕB=0), and 4th is Faraday's Law (тИЗ├ЧEтГЧ=тИТтИВBтГЧтИВt\nabla \times \vec{E} = -\frac{\partial\vec{B}}{\partial t}тИЗ├ЧE=тИТтИВtтИВBтАЛ).

Related Questions

ElectricalElectromagnetics Field Theory
For air, the Maxwell's equation hold true is
ElectricalElectromagnetics Field Theory
For any metals, the Maxwell's equation hold true is
ElectricalElectromagnetics Field Theory
MaxwellтАЩs equation not be represented in
ElectricalElectromagnetics Field Theory
Maxwell's equation derived from AmpereтАЩs law is
ElectricalElectromagnetics Field Theory
Maxwell's equation derived from FaradayтАЩs law is

Discussion (0)

Loading discussion...
PrevNext