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ElectricalElectromagnetics Field Theory
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MaxwellтАЩs first equation in free space is

A

тИЗ├ЧH=J+тИВDтИВt\nabla \times H = J + \frac{\partial D}{\partial t}тИЗ├ЧH=J+тИВtтИВDтАЛ

B

тИЗ├ЧH=тИВDтИВt\nabla \times H = \frac{\partial D}{\partial t}тИЗ├ЧH=тИВtтИВDтАЛ

C

тИЗ├ЧH=0\nabla \times H = 0тИЗ├ЧH=0

D

тИЗ├ЧH=J\nabla \times H = JтИЗ├ЧH=J

Correct Answer

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

тИЗ├ЧH=тИВDтИВt\nabla \times H = \frac{\partial D}{\partial t}тИЗ├ЧH=тИВtтИВDтАЛ

Quick Summary:

MaxwellтАЩs first equation, derived from the Ampere-Maxwell Law, relates the magnetic field intensity to the displacement current density in the absence of conduction currents. In free space, where the conductivity ╧Г=0\sigma = 0╧Г=0, the conduction current density J=0J = 0J=0, leading to the relation тИЗ├ЧH=тИВDтИВt\nabla \times H = \frac{\partial D}{\partial t}тИЗ├ЧH=тИВtтИВDтАЛ.

тЪЩя╕ПTETechnical SolutionConcept & Principle
ЁЯТб Explanation

MaxwellтАЩs first equation, derived from the Ampere-Maxwell Law, relates the magnetic field intensity to the displacement current density in the absence of conduction currents. In free space, where the conductivity ╧Г=0\sigma = 0╧Г=0, the conduction current density J=0J = 0J=0, leading to the relation тИЗ├ЧH=тИВDтИВt\nabla \times H = \frac{\partial D}{\partial t}тИЗ├ЧH=тИВtтИВDтАЛ.

ЁЯФв Key Formulas

тИЗ├ЧH=J+тИВDтИВt\nabla \times H = J + \frac{\partial D}{\partial t}тИЗ├ЧH=J+тИВtтИВDтАЛ тАФ General Ampere-Maxwell Law

тИЗ├ЧH=тИВDтИВt\nabla \times H = \frac{\partial D}{\partial t}тИЗ├ЧH=тИВtтИВDтАЛ тАФ Free space condition

тЪЩя╕П Working Principle

The principle stems from the generalization of Ampere's Law to include time-varying electric fields. Faraday's discovery of electromagnetic induction necessitated the addition of the displacement current term, тИВDтИВt\frac{\partial D}{\partial t}тИВtтИВDтАЛ, to maintain the consistency of the continuity equation. In a vacuum (free space), charge density ╧Б=0\rho = 0╧Б=0 and current density J=0J = 0J=0, making the time-variation of the electric displacement field the sole source of the circulating magnetic field.

ЁЯУМ Key Points
  • тЦ╕

    Maxwell's equations are the foundation of classical electromagnetism.

  • тЦ╕

    The term тИВDтИВt\frac{\partial D}{\partial t}тИВtтИВDтАЛ represents the displacement current density.

  • тЦ╕

    In free space, conductivity is zero, hence J=0J=0J=0.

  • тЦ╕

    This equation implies that a time-varying electric field generates a magnetic field.

тЬЕ Advantages
  • тЦ╕

    Predicts electromagnetic wave propagation.

  • тЦ╕

    Provides a unified theory for electric and magnetic fields.

тЭМ Disadvantages / Limitations
  • тЦ╕

    Does not account for quantum electrodynamic effects.

  • тЦ╕

    Requires knowledge of vector calculus for implementation.

ЁЯЫая╕П Applications / Uses
  • тЦ╕

    Radio wave transmission.

  • тЦ╕

    Design of antennas and waveguides.

ЁЯУД Additional Information
  • тЦ╕

    The constant ╧╡0\epsilon_0╧╡0тАЛ is the permittivity of free space, approximately 8.854├Ч10┬░тИТ12┬аF/m8.854 \times 10┬░{-12} \text{ F/m}8.854├Ч10┬░тИТ12┬аF/m.

  • тЦ╕

    Option A is the general form including conduction current JJJ. Option C represents a static field without time variation. Option D is Ampere's law for static currents (magnetostatics).

ЁЯУК Diagram / Illustration
Maxwell's First Equation (Free Space)
тИЗ├ЧH=тИВDтИВt\nabla \times H = (\partial D / \partial t)тИЗ├ЧH=тИВtтИВDтАЛ
Where D=╧╡0ED = \epsilon_0 ED=╧╡0тАЛE
and J=0J = 0J=0 in free space
тЬЕ

B is correct тАФ In free space, the conduction current density JJJ is zero, simplifying the Maxwell-Ampere equation to the curl of the magnetic field intensity equal to the time derivative of the electric displacement field тИЗ├ЧH=тИВDтИВt\nabla \times H = \frac{\partial D}{\partial t}тИЗ├ЧH=тИВtтИВDтАЛ.

Core Concepts Used
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Ampere-Maxwell Law Displacement Current Electromagnetic Fields
ЁЯТб EXAM TIP

Always verify the medium conditions (e.g., free space, conductor, or dielectric) before applying Maxwell's equations, as JJJ and ╧Б\rho╧Б variations change the equation form significantly.

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