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The electric field in dielectrics The electric field in dielectrics

The electric field in dielectrics - PowerPoint Presentation

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Uploaded On 2018-11-21

The electric field in dielectrics - PPT Presentation

Section 6 Dielectrics C onstant currents are impossible Constant internal electric fields are possible No macroscopic currents Macroscopic field Might be locally nonzero Neutral dielectric Includes only charges belonging to dielectric namely electrons and protons of neutral constitu ID: 731264

charge dielectric electric density dielectric charge density electric dielectrics extraneous conductor neutral total boundary surface units charges component moment div dipole field

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Presentation Transcript

Slide1

The electric field in dielectrics

Section 6Slide2

Dielectrics:

C

onstant currents are impossibleConstant internal electric fields are possible.

No macroscopic currents

Macroscopic field

Might be locally non-zeroSlide3

Neutral dielectric: Includes only charges belonging to dielectric, namely electrons and protons of neutral constituent atoms

Total charge =

Hence

where

P

= 0 outside the dielectric

Over volume of dielectric

On boundary that surrounds dielectric

since

P

= 0 outside the dielectricProof P is the “dielectric polarization” or “polarization”. If non-zero, body is “polarized”.Slide4

The component of P along the outward normal =

P

n

=

P.n

= sSlide5

Total dipole moment of the dielectric

i

th

component

surface

Sum over j

Dipole moment =

= dipole moment per unit volumeSlide6

Still talking about neutral dielectrics

Holds both inside and outside (where

D

=

E

)

“Electric induction”

Average <

r

>

r is over charges belonging to the dielectricSlide7

If extraneous charges are added, we get a “charged” dielectric

Extraneous charge densitySlide8

Boundary between two

dielectrics

E

1t = E2tTangential component of electric field is continuous

=

E

1

E

2Slide9

Boundary between two dielectrics

D

1

If

D

n

=

D

z

were discontinuous, then

which would contradictSlide10

Boundary between dielectric and conductor

E

t = 0 in the conductor

Curl E = 0 still holdsEt is continuousTherefore Et = 0 on both sidesSlide11

Even a neutral conductor can have surface charge (but no

P

)

Surface charge density on conductor = extraneous charge on dielectric

dielectric

conductorSlide12

Name and unit conventions

Landau, Gaussian Units

D

= E + 4 p P = electric induction

D,E,P all have the same unitsDiv D = 4 p rex

(extraneous charge density)

Div E = 4 p <r>r (total charge density, intrinsic + extraneous)

Other books, S.I. unitsD = e0E + P = electric

displacementD,P have the same units, E has different units (V/m)Div D = rf

(free charge density)Div

E = r/e0 (total charge density, bound+ free)