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Bound charge and bound current

Polarization and magnetization produce the effective sources

ρ_{b} = - \nabla \cdot P, J_{b} = \partial_{t} P + \nabla \times M .

Defining

D = ϵ_{0} E + P

and

H = B / μ_{0} - M

moves these sources into the macroscopic fields.

Table of contents 161 4
- Electric polarization Bound charge and bound current 71 1
  - Electric displacement field Electric polarization 23
- Magnetization Bound charge and bound current 65 1
  - Magnetic field intensity Magnetization 26

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