Properties of Electromagnetic Waves
Electromagnetic Waves • Properties • Premium Physics Notes

Properties of Electromagnetic Waves

Understand transverse nature, E ⊥ B relation, velocity of EM waves, E₀/B₀ = c, polarisation, energy density, Poynting vector, momentum, radiation pressure and advanced numerical applications.

Still Confused in Electromagnetic Waves?

If transverse nature, E ⊥ B relation, polarisation, radiation pressure, momentum, energy density or EM-wave numericals are not clear, students can contact Kumar Sir for one-to-one Physics guidance.

Kumar Physics Classes

Phone / WhatsApp: +91-9958461445

Website: https://kumarphysicsclasses.com

Email: kumarsirphysics@gmail.com

Section 1: Introduction to EM Waves

Electromagnetic waves are waves of oscillating electric and magnetic fields. Maxwell predicted that a changing electric field produces a magnetic field and a changing magnetic field produces an electric field. This self-sustaining mechanism allows EM waves to travel even through vacuum.

Mechanical waves
Require a material medium. Sound waves need air, water or solid particles for propagation.
Electromagnetic waves
Do not require a material medium. Light from the Sun reaches Earth through vacuum because EM waves are field waves.
Propagation +x E along y-axis B along z-axis E, B and propagation are mutually perpendicular; E × B gives wave direction.

Section 2: Transverse Nature of EM Waves

EM waves are transverse because both electric and magnetic fields oscillate perpendicular to the direction of propagation. A longitudinal EM wave in vacuum is impossible because Maxwell equations require the fields to be divergence-free away from charges and perpendicular to the direction of energy flow.

E ⊥ B
E ⊥ direction
B ⊥ direction
E ⊥ B ⊥ c
Concept Example 1
If propagation is +x and E is +y, then B must be +z.
Concept Example 2
If propagation is +z and E is +x, then B must be +y.
Concept Example 3
If E and B are parallel, E × B = 0, so there is no propagation direction.

Section 3: E ⊥ B ⊥ Direction of Propagation

For propagation along +x direction:

Ey = E0 sin(kx - ωt) Bz = B0 sin(kx - ωt)

Electric field is along y-axis, magnetic field is along z-axis and propagation is along x-axis. The right-hand rule gives E × B = direction of propagation.

+x propagation E (+y) B (+z) Right-hand rule: curl E toward B; thumb gives propagation.

Section 4: Velocity of Electromagnetic Waves

Vacuum

c = 1 / √(μ0ε0)

Substituting μ0 = 4π × 10-7 and ε0 = 8.854 × 10-12 gives c ≈ 3 × 108 m/s.

Medium

v = 1 / √(με)

In a medium, permeability μ and permittivity ε determine the wave speed, so v is generally less than c.

Physical significance: Maxwell's value matched the speed of light, proving that light is an electromagnetic wave. Radio waves, microwaves, visible light, X-rays and gamma rays all travel at c in vacuum.

Section 5: Relation E₀/B₀ = c

Amplitude Relation

E0 = cB0E0/B0 = c
Meaning:
E0 is the electric field amplitude in V/m. B0 is the magnetic field amplitude in tesla. Their ratio is the speed of the wave in vacuum.
Unit analysis: (V/m)/T = (N/C)/(N/(A m)) = A m/C = m/s because A = C/s.

Section 6: Energy Density of EM Waves

ElectricUE = 1/2 ε0
MagneticUB = B²/(2μ0)
Equal sharingUE = UB
TotalU = UE + UB = ε0

Using E = cB and c² = 1/(μ0ε0), electric and magnetic energy densities become equal. This means energy is equally shared between electric and magnetic fields.

Section 7: Poynting Vector

S = (E × B)/μ0

The Poynting vector gives the rate of energy flow per unit area. Its direction is the direction of propagation and its SI unit is W/m².

E B S = E × B / μ₀

Section 8: Polarisation

Polarisation is the restriction of vibrations of a transverse wave to one plane. Only transverse waves can be polarised, so polarisation is strong evidence that electromagnetic waves are transverse.

Polariser
Allows only one component of the electric field to pass.
Proof of transverse nature
Longitudinal waves cannot be polarised because their oscillations are along propagation.
Applications
Polarised sunglasses, LCD displays, photography filters, stress analysis and glare reduction.
Unpolarised transverse components Polariser Plane-polarised light

Section 9: Momentum of Electromagnetic Waves

Electromagnetic waves carry energy and momentum. For photons and radiation, energy and momentum are related by:

E = pc

When EM waves are absorbed or reflected, they transfer momentum to the surface. This momentum transfer causes radiation pressure.

Section 10: Radiation Pressure

Absorbing surfaceP = I/c
Reflecting surfaceP = 2I/c
Force absorbingF = IA/c
Force reflectingF = 2IA/c

Here I is intensity in W/m², A is area in m², c is speed of light and P is radiation pressure in N/m².

Section 11: Solved Numericals

Section 12: PYQs

Section 13: Case Studies

Section 14: Important Conceptual Questions

Section 15: Common Mistakes

Confusing E and B direction
Always use E × B to get propagation direction.
Wrong right-hand rule
Curl fingers from E to B, not from B to E.
Forgetting E₀/B₀ = c
This relation is for field amplitudes in vacuum.
Confusing intensity and energy density
Intensity is power per unit area; energy density is energy per unit volume.
Wrong pressure formula
Absorbing surface uses I/c; reflecting surface uses 2I/c.
Wrong photon relation
For EM radiation, energy and momentum follow E = pc.
Mixing absorbing and reflecting force
Use F = IA/c for absorption and F = 2IA/c for reflection.

Section 16: Final Revision Sheet

E ⊥ B ⊥ c
c = 1/√(μ₀ε₀)
v = 1/√(με)
E₀ = cB₀
E₀/B₀ = c
UE = 1/2 ε₀E²
UB = B²/2μ₀
UE = UB
U = ε₀E²
S = (E × B)/μ₀
E = pc
Pabs = I/c
Pref = 2I/c
Fabs = IA/c
Fref = 2IA/c

Still Confused in Electromagnetic Waves?

If transverse nature, E ⊥ B relation, polarisation, radiation pressure, momentum, energy density or EM-wave numericals are not clear, students can contact Kumar Sir for one-to-one Physics guidance.

Kumar Physics Classes

Phone / WhatsApp: +91-9958461445

Website: https://kumarphysicsclasses.com

Email: kumarsirphysics@gmail.com

Properties of Electromagnetic Waves

Properties of Electromagnetic Waves

5.10 Important Characteristics and Properties of Electromagnetic Waves

5.10 Important Characteristics and Properties of Electromagnetic Waves

Properties of Electromagnetic Waves

1. Production of Electromagnetic Waves

Electromagnetic waves are produced by accelerated or oscillating charges.

2. No Material Medium Required

Electromagnetic waves do not require any material medium for propagation and can travel through vacuum.

3. Speed of Electromagnetic Waves in Free Space

Electromagnetic waves travel in free space with the speed of light:

c = 3 × 108 m s−1

where

c = 1√(μ0 ε0)

Here,

  • ( μ0 ) = Permeability of free space
  • ( ε0 ) = Permittivity of free space

4. Electric and Magnetic Fields Oscillate Simultaneously

In an electromagnetic wave, both electric field (E) and magnetic field (B) vary sinusoidally and simultaneously.

Therefore:

  • Maximum values occur at the same place and at the same time.
  • Minimum values occur at the same place and at the same time.

The amplitudes are related by:

E0B0 = c

or

E0 = cB0

5. Direction of Propagation

The direction of propagation of an electromagnetic wave is given by the cross product:

S = E × Bμ0

where (S) is the Poynting Vector.

Thus,

E × B

gives the direction of wave propagation.

6. Electromagnetic Waves are Transverse Waves

The electric field, magnetic field, and direction of propagation are mutually perpendicular.

EB
E ⟂ Direction of Propagation
B ⟂ Direction of Propagation

Hence electromagnetic waves are transverse in nature.

7. Velocity Depends on Medium

The velocity of electromagnetic waves depends only on the electrical and magnetic properties of the medium.

It is independent of the amplitudes of electric and magnetic fields.

For a medium:

v = 1√(μ ε)

8. Velocity in Dielectric Medium

The speed of electromagnetic waves in a dielectric medium is less than the speed of light in vacuum.

v<c
v < 3 × 108 m s−1

9. Equal Distribution of Energy

Electromagnetic waves carry energy.

This energy is equally divided between:

  • Electric field energy
  • Magnetic field energy

Thus,

uE = uB

Energy Density of Electromagnetic Waves

Electric Energy Density

uE = 12 ε0E2

Magnetic Energy Density

uB = 10B2

Total Energy Density

u = uE + uB
u = 12 ε0E2 + 10B2

For Electromagnetic Waves (Using RMS Values)

Since electric and magnetic fields vary sinusoidally, RMS values are used.

Erms = E0√2
Brms = B0√2

Average Electric Energy Density

uE = 12 ε0Erms2
uE = 12 ε0(E0√2)2
uE = 14 ε0E02

Average Magnetic Energy Density

uB = 10Brms2
uB = 10(B0√2)2
uB = 10B02

Using

E0B0 = c

and

c2 = 1μ0ε0

we get

uB = 10(E0c)2
uB = ε0E024

Therefore,

uB = uE

Important Result

uE = uB

Hence,

u = uE + uB
u = 2uE = 2uB
u = 12 ε0E02

or

u = B020

Quick Revision

  • EM waves are produced by accelerated charges.
  • No material medium is required.
  • Speed in vacuum:
c = 1√(μ0ε0)
  • Electric and magnetic fields are in phase.
  • (E0/B0 = c)
  • ( EB ⟂ ) direction of propagation.
  • EM waves are transverse.
  • (uE = uB)
  • Total energy density:
u = uE + uB
  • Poynting Vector:
S = E × Bμ0
  • Energy is equally shared between electric and magnetic fields.
Scroll to Top