I_d = epsilon0 (d(Phi_E)/dt)
Displacement current equals permittivity of free space times the rate of change of electric flux.
Displacement current is proportional to the rate of change of electric flux.
- I_d
- displacement current (A)
- epsilon0
- permittivity of free space (F/m)
- Phi_E
- electric flux (V·m)
Use when — The electric field between the plates of a capacitor or in a similar region is changing with time.
Common trap — Treating displacement current as a flow of charge across the gap.
closed-loop integral of B dot dl = mu0 (I + I_d)
The closed loop integral of magnetic field equals permeability of free space times the sum of conduction current and displacement current.
The Ampere-Maxwell law adds displacement current to conduction current as a source of magnetic field.
- B
- magnetic field (T)
- I
- conduction current (A)
- mu0
- permeability of free space (T·m/A)
Use when — A region has both conduction current and a changing electric field.
Common trap — Dropping the displacement current term when the electric field is time-varying.
c = 1 / sqrt(mu0 * epsilon0)
Speed of light in vacuum equals one over the square root of the product of permeability and permittivity of free space.
The speed of an electromagnetic wave in vacuum is fixed by the permeability and permittivity of free space.
- c
- speed of light in vacuum (m/s)
- mu0
- permeability of free space (T·m/A)
- epsilon0
- permittivity of free space (F/m)
Use when — The wave travels through vacuum, or free space is a valid approximation.
Common trap — Applying this vacuum-only relation directly inside a material medium.
v = 1 / sqrt(mu * epsilon)
Speed in a medium equals one over the square root of the product of the medium's permeability and permittivity.
The speed of an electromagnetic wave in a medium depends on that medium's permeability and permittivity.
- v
- speed in the medium (m/s)
- mu
- permeability of the medium (T·m/A)
- epsilon
- permittivity of the medium (F/m)
Use when — The wave travels through a specified material medium rather than vacuum.
Common trap — Using vacuum values of permeability and permittivity for a medium.
E0 / B0 = c
The ratio of peak electric field to peak magnetic field equals the speed of light.
The peak electric field and peak magnetic field of a vacuum electromagnetic wave stay in a fixed ratio equal to the speed of light.
- E0
- peak electric field (V/m)
- B0
- peak magnetic field (T)
Use when — The wave is travelling in vacuum and both peak field magnitudes are being related.
Common trap — Assuming E0 and B0 are numerically equal instead of related through the speed of light.
u_avg = (1/2) epsilon0 E0^2
Average energy density equals one half permittivity of free space times the square of the peak electric field.
The average energy density of a vacuum electromagnetic wave, combining equal electric and magnetic contributions.
- u_avg
- average energy density (J/m^3)
- E0
- peak electric field (V/m)
Use when — The electric and magnetic contributions to stored energy are being combined for a vacuum wave.
Common trap — Counting only the electric field contribution and ignoring the equal magnetic contribution.
I = u_avg * c
Intensity equals average energy density times the speed of light.
Intensity is the rate of energy transfer per unit area, obtained from the average energy density and the wave speed.
- I
- intensity (W/m^2)
- u_avg
- average energy density (J/m^3)
- c
- speed of light in vacuum (m/s)
Use when — The rate of energy delivery per unit area is required for a vacuum electromagnetic wave.
Common trap — Confusing intensity with total energy rather than energy per unit area per unit time.
p = U / c
Momentum delivered equals energy delivered divided by the speed of light.
At the elementary syllabus level, the momentum delivered by a fully absorbed electromagnetic wave equals the energy delivered divided by the speed of light.
- p
- momentum delivered (kg·m/s)
- U
- energy delivered (J)
- c
- speed of light in vacuum (m/s)
Use when — The surface fully absorbs the incident wave, at the elementary qualitative level the syllabus specifies.
Common trap — Applying this absorption relation to a fully reflecting surface without doubling the momentum transfer.