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Electrostatics Magnetostatics

Stationary charges ⇒ Constant Electric Steady currents ⇒ Constant

Coulomb’s Law Biot-Savart’s Law

1 ̂ ̂ 4 4

(Inverse Square Law) (Inverse Square Law)

Electric field is the negative of the Magnetic field is the of magnetic vector electric . potential.

1 ′ ′ ′ ′ 4 |′| 4 |′|

Electric Scalar Potential Magnetic Vector Potential

Three Poisson’s equations for solving Poisson’s equation for solving electric scalar magnetic vector potential potential.

Discrete 2 Physical ′′′ Continuous

Magnetic Dipole Moment

1 1 1 3 ∙̂̂ 3 ∙̂̂ 4 4

Electric field cause by an electric dipole Magnetic field cause by a

Torque on an electric dipole Torque on a magnetic dipole

∙ ∙

Electric on an electric dipole Magnetic force on a magnetic dipole

∙ ∙

Electric Magnetic Potential Energy of an electric dipole of a magnetic dipole

Electric Dipole Moment per unit volume Magnetic Dipole Moment per unit volume (Polarisation) (Magnetisation)

Volume Bound Volume Bound

Surface Bound Charge Density Surface Bound Current Density

Volume Charge Density Volume Current Density

Net , Free , Bound Net , Free , Bound

Volume Charge Volume Current

Net , Free , Bound Net ,Free , Bound

1

= Electric field = Magnetic field = Electric Displacement = Auxiliary Field = Polaristion = Magnetic

Polarisation is proportional to the electric field. Magnetization is proportional to the magnetic field. (Provided the electric field is not too strong) (Provided the magnetic field is not too strong)

Note: Notice that the in is replaced by 1/ and not 1/ in

in dielectric material 1/ in magnetic material in free space 1/ in free space

1 1

of dielectric Permeability of material Permittivity of free space Permeability of free space Relative Permeability Electric Susceptibility Note: Note:  ϵ,ϵ0  , 0

 Electric Susceptibility is a dimensionless  Magnetic Susceptilibity is a dimensionless proportionality constant that indicates the proportionality constant that indicates the degree degree of polarization of a dielectric material in of magnetization of a magnetic material in response to an applied electric field. response to an applied magnetic field.

 0 0 paramagnet M parallel  0 diamagnet M parallel  1 1 paramagnet M parallel  1 diamagnet M parallel

Gauss’s law on net charges ’s law on net current

‐ ‐ ‐ ‐ ∙ ∙ ∙

Differential Differential Integral

= Electric field = Magnetic field

Gauss’s law on bound charges ’s law on bound current

‐ ‐ ‐ ‐ ∙ ∙ ∙

Differential Integral Differential Integral

= Dielectric Polaristion = Magnetic Magnetization

Gauss’s law on free charges Amperes’s law on free current

‐ ‐ ‐ ∙ ∙ ∙

Differential Integral Differential Integral

= Electric Displacement = Auxiliary Field

Maxwell’s Equations

Gauss’s law on Gaussian Surface Amperes’s law on Amperian Loop

∙ ∙ ∙

Differential Integral Differential Integral

Electric diverges away from (towards to) a positive Magnetic field line curls around current. (negative) charge.

Differential Integral Differential Integral

0 ∙ 0 ∙ 0 ∙ 0

Electrostatic field line does not curl, it diverges. Magnetic field line curls & loop. It does not diverges. No magnetic monopole.

Lorentz Force