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ElectricalElectromagnetics Field Theory
PrevNext

The charge build up in a capacitor is due to

A

Conduction current density

B

Displacement current density

C

Polarization

D

Magnetization

Correct Answer

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

Displacement current density

Quick Summary:

The charge buildup on capacitor plates in a time-varying field is driven by displacement current, as defined in Maxwell's modification to Ampere's Law. Even though no physical charge carriers cross the dielectric gap, the changing electric flux creates an effective current.

тЪЩя╕ПTETechnical SolutionConcept & Principle
ЁЯТб Explanation

The charge buildup on capacitor plates in a time-varying field is driven by displacement current, as defined in Maxwell's modification to Ampere's Law. Even though no physical charge carriers cross the dielectric gap, the changing electric flux creates an effective current.

ЁЯФв Key Formulas

Jd=тИВDтГЧтИВtJ_d = \frac{\partial\vec{D}}{\partial t}JdтАЛ=тИВtтИВDтАЛ тАФ Definition of displacement current density

DтГЧ=╧╡EтГЧ\vec{D} = \epsilon\vec{E}D=╧╡E тАФ Relationship between flux density and electric field

тЪЩя╕П Working Principle

In a capacitor, the time-varying electric field EтГЧ\vec{E}E produces a changing electric flux density DтГЧ\vec{D}D. Maxwell's fourth equation states that тИЗ├ЧHтГЧ=JтГЧc+тИВDтГЧтИВt\nabla \times \vec{H} = \vec{J}_c + \frac{\partial\vec{D}}{\partial t}тИЗ├ЧH=JcтАЛ+тИВtтИВDтАЛ. The term тИВDтГЧтИВt\frac{\partial\vec{D}}{\partial t}тИВtтИВDтАЛ represents the displacement current density (JdJ_dJdтАЛ), which accounts for the accumulation of charge on the metallic plates despite the presence of an insulating dielectric.

ЁЯУМ Key Points
  • тЦ╕

    Displacement current is not a flow of charge carriers like conduction current.

  • тЦ╕

    It is proportional to the time rate of change of the electric field intensity.

  • тЦ╕

    It allows the continuity of current in circuits containing capacitors.

  • тЦ╕

    It satisfies the condition for the continuity equation тИЗтЛЕJтГЧ+тИВ╧БvтИВt=0\nabla \cdot \vec{J} + \frac{\partial \rho_v}{\partial t} = 0тИЗтЛЕJ+тИВtтИВ╧БvтАЛтАЛ=0.

тЬЕ Advantages
  • тЦ╕

    Enables existence of electromagnetic waves in free space

  • тЦ╕

    Essential for analyzing high-frequency circuit behavior

тЭМ Disadvantages / Limitations
  • тЦ╕

    Does not contribute to ohmic heating (Joule heating) in dielectrics

  • тЦ╕

    Often neglected in DC steady-state analysis

ЁЯЫая╕П Applications / Uses
  • тЦ╕

    Electromagnetic wave propagation theory

  • тЦ╕

    Capacitor charge-discharge analysis in AC circuits

ЁЯУД Additional Information
  • тЦ╕

    Conduction current density refers to the flow of free electrons in a conductor.

  • тЦ╕

    Magnetization describes the density of magnetic dipole moments in a material, which does not cause plate charge accumulation.

  • тЦ╕

    Polarization (PPP) refers to the alignment of dipoles in a dielectric, which is related to DDD (D=╧╡0E+PD = \epsilon_0 E + PD=╧╡0тАЛE+P) but is distinct from the current causing charge transport.

ЁЯУК Diagram / Illustration
Displacement Current Density
тИВDтГЧтИВt\frac{\partial\vec{D}}{\partial t}тИВtтИВDтАЛ
JdJ_dJdтАЛ (Amperes per square meter)
Mathematical representation of displacement current
тЬЕ

B is correct тАФ The displacement current density тИВDтГЧтИВt\frac{\partial\vec{D}}{\partial t}тИВtтИВDтАЛ provides a physical mechanism for the continuity of current through capacitors, resulting in the accumulation of charge.

Core Concepts Used
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Maxwell's Equations Ampere's Circuital Law Displacement Current
ЁЯТб EXAM TIP

Remember that displacement current is the vital link that makes Maxwell's equations consistent with the charge conservation principle (nablacdotvecJ=тИТfracpartialrhopartialt\\nabla \\cdot \\vec{J} = -\\frac{\\partial \\rho}{\\partial t}nablacdotvecJ=тИТfracpartialrhopartialt).

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