Q.In a plane electromagnetic wave, the electric field oscillates sinusoidally at a frequency of 2.0×1010 Hz and amplitude 48 V m−1.
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🔒 Start your 14-day free trial to unlock the full solution →Concept understanding — Electromagnetic Wave Relation
Electromagnetic Wave Relation: From Intuition to Precision
Imagine you're standing at the beach. You see a wave coming in — it has a certain speed, a certain distance between crests (wavelength), and a certain number of crests passing you per second (frequency). The faster the wave, the more crests pass you in a given time. That's the basic idea: speed = frequency × wavelength.
Now, light is also a wave — an electromagnetic wave. It doesn't need water or air; it travels through empty space at a staggering speed. The relation that governs all waves, including light, is:
v=fλ
where v is the wave speed, f is the frequency (in hertz, Hz), and λ (lambda) is the wavelength (in metres).
For electromagnetic waves in vacuum, this speed is a universal constant: c=3×108 m/s. So the relation becomes:
c=fλ
That's it. But let's unpack what this really means.
What is frequency? What is wavelength?
Frequency is how many complete wave cycles pass a fixed point in one second. A radio station broadcasting at 100 MHz means 100 million cycles per second. Higher frequency means more oscillations per second.
Wavelength is the distance between two consecutive crests (or troughs) of the wave. For visible light, wavelengths are tiny — around 400 to 700 nanometres (billionths of a metre).
The product fλ always equals the wave speed. So if frequency goes up, wavelength must go down to keep the product constant. This is why:
- Gamma rays have extremely high frequency and extremely short wavelength.
- Radio waves have low frequency and very long wavelength (metres to kilometres).
Both travel at the same speed c in vacuum.
Why does this matter for exams?
You'll use this relation in three main ways:
- Given frequency, find wavelength (or vice versa) — just rearrange: λ=fc or f=λc.
- Compare different regions of the electromagnetic spectrum — know that as frequency increases, wavelength decreases proportionally.
- Solve problems involving energy — because photon energy E=hf (where h is Planck's constant), the wave relation links energy to wavelength: E=λhc.
A common mistake: using c=fλ for waves in a medium (like glass or water). In a medium, the speed is less than c, so the wavelength changes but frequency stays the same. The relation v=fλ still holds, but v is now the speed in that medium.
A concrete example
A microwave oven operates at 2.45 GHz. What is its wavelength in vacuum?
f=2.45×109 Hz, c=3×108 m/s. …
Why this formula?
Electromagnetic Wave Relation: Why c=μ0ε01
Let's build this from first principles — not just memorising the formula, but understanding why light and all EM waves travel at this specific speed.
1. The Starting Point: Maxwell's Equations in Vacuum
In empty space (no charges, no currents), Maxwell's equations simplify to:
- Gauss's law for electricity: ∇⋅E=0
- Gauss's law for magnetism: ∇⋅B=0
- Faraday's law: ∇×E=−∂t∂B
- Ampère-Maxwell law: ∇×B=μ0ε0∂t∂E
The key insight: a changing electric field creates a magnetic field, and a changing magnetic field creates an electric field. This mutual induction is what sustains the wave.
2. Deriving the Wave Equation for E
Take the curl of Faraday's law:
∇×(∇×E)=∇×(−∂t∂B)=−∂t∂(∇×B)
Now use the vector identity: ∇×(∇×E)=∇(∇⋅E)−∇2E
Since ∇⋅E=0 in vacuum, this becomes:
−∇2E=−∂t∂(∇×B)
Substitute ∇×B from Ampère-Maxwell:
−∇2E=−∂t∂(μ0ε0∂t∂E)
Result: The electric field satisfies the wave equation:
∇2E=μ0ε0∂t2∂2E
3. Identifying the Wave Speed
Compare with the standard wave equation for any wave travelling at speed v:
∇2ψ=v21∂t2∂2ψ
Matching terms:
v21=μ0ε0⇒v=μ0ε01
This v is the speed of electromagnetic waves in vacuum — denoted c.
Why this is profound: The constants μ0 (permeability of free space) and ε0 (permittivity of free space) come from static electricity and magnetism. Yet their combination gives the speed of light — showing light is an electromagnetic wave.
4. The Magnetic Field Follows Suit
Exactly the same derivation starting from Ampère-Maxwell law gives:
∇2B=μ0ε0∂t2∂2B
So both E and B propagate at the same speed c.
5. The Crucial Relationship Between E and B
For a plane wave travelling in the x-direction:
- E oscillates along y: Ey=E0sin(kx−ωt)
- B oscillates along z: Bz=B0sin(kx−ωt)
From Faraday's law: ∂x∂Ey=−∂t∂Bz
Differentiating the wave forms:
kE0cos(kx−ωt)=ωB0cos(kx−ωt)
Since ω=ck, we get:
B0E0=kω=c …
Concept: Electromagnetic Wave Relation — in a vacuum, c=fλ and E0=cB0, with equal average energy densities in the electric and magnetic fields.
(a) Wavelength:
λ=fc=2.0×10103×108=1.5×10−2 m
(b) Magnetic field amplitude:
B0=cE0=3×10848=1.6×10−7 T
(c) Average energy densities:
uE=21ε0E02×21=41ε0E02,uB=2μ01B02×21=4μ01B02 …
For a plane EM wave, the wavelength is found from c=fλ, the magnetic amplitude from E0=cB0, and the equality of average energy densities follows from uE=21ε0E2 and uB=2μ0B2 together with c=1/μ0ε0.
This is a classic problem that tests your understanding of the fundamental relationships in an electromagnetic wave. In free space, the electric and magnetic fields are not independent — they are linked by the speed of light, and their energy densities are always equal on average. Let’s see why.
1. Wavelength from frequency
For any wave, the speed, frequency, and wavelength are related by v=fλ. For an electromagnetic wave in vacuum, v=c.
Given:
- f=2.0×1010 Hz
- c=3×108 m s−1
So:
λ=fc=2.0×10103×108=1.5×10−2 m
That’s 1.5 cm — a microwave wavelength.
Notice the frequency is 2×1010 Hz, which is 20 GHz — right in the microwave band. The wavelength of 1.5 cm confirms this.
2. Magnetic field amplitude from electric field amplitude
In a plane EM wave, the instantaneous magnitudes are related by E=cB. This holds for the amplitudes too:
E0=cB0
Given E0=48 V m−1:
B0=cE0=3×10848=1.6×10−7 T
A common mistake is to forget that B0 is in tesla, not gauss. 1.6×10−7 T is 1.6 milligauss — a very small field, which is typical for EM waves.
3. Showing that average energy densities are equal
The instantaneous energy densities are:
- Electric: uE=21ε0E2
- Magnetic: uB=2μ0B2
For a sinusoidal wave, E=E0sin(kx−ωt) and B=B0sin(kx−ωt). The time average of sin2 over one cycle is 1/2.
So:
⟨uE⟩=21ε0⟨E2⟩=21ε0⋅2E02=41ε0E02 …
Method: Standard Wave Relations for EM Waves
This problem uses the fundamental wave equation and the intrinsic relation between E and B in free space, plus the energy density equality property of EM waves.
(a) Wavelength of the wave
Step 1: Recall the wave equation
For any electromagnetic wave in vacuum:
c=νλ
Step 2: Substitute given values
λ=νc=2.0×10103×108
Step 3: Compute
λ=1.5×10−2 m
Answer: 1.5×10−2 m (or 1.5 cm)
(b) Amplitude of the magnetic field
Step 1: Use the E–B amplitude relation in free space
E0=cB0
Step 2: Rearrange and substitute
B0=cE0=3×10848
Step 3: Compute
B0=1.6×10−7 T
Answer: 1.6×10−7 T
(c) Show average energy densities are equal
Step 1: Write the average energy density formulas
- Electric field:
⟨uE⟩=21ε0⟨E2⟩=41ε0E02
- Magnetic field:
⟨uB⟩=21μ0⟨B2⟩=41μ0B02
Step 2: Use B0=E0/c and c=1/ε0μ0
Substitute into ⟨uB⟩: …
Common Mistakes & How to Avoid Them
Mistake 1: Using wrong formula for wavelength
The error: Students often confuse c=fλ with v=fλ and forget that for EM waves in vacuum, v=c.
How to avoid: Always write the relation explicitly:
c=fλ
Then rearrange:
λ=fc=2.0×10103×108=1.5×10−2 m
Key check: The answer should be in metres — if you get a tiny number like 1.5 cm, that's correct for such a high frequency.
Mistake 2: Forgetting the factor of c in E0 and B0 relation
The error: Students write E0=B0 or E0=cB0 incorrectly (swapping numerator/denominator).
How to avoid: Memorise the exact relation:
c=B0E0⇒B0=cE0
So:
B0=3×10848=1.6×10−7 T
Quick sanity check: B0 is always much smaller than E0 (by factor c), so 10−7 T is reasonable.
Mistake 3: Using wrong formula for energy density
The error: Students use uE=21ε0E2 but forget the average value, or use peak value E0 instead of RMS value.
How to avoid: For sinusoidal variation:
- Instantaneous: uE=21ε0E2
- Average over one cycle: ⟨uE⟩=41ε0E02
Similarly for magnetic field:
- Instantaneous: uB=2μ0B2
- Average: ⟨uB⟩=4μ0B02
Mistake 4: Not proving equality — just stating it
The error: Students write "they are equal" without showing the algebra.
How to avoid: Show the derivation step-by-step:
- Write ⟨uE⟩=41ε0E02
- Write ⟨uB⟩=4μ0B02
- Substitute B0=E0/c and c=1/μ0ε0: ⟨uB⟩=4μ0(E0/c)2=4μ0c2E02=4μ0⋅μ0ε01E02=41ε0E02=⟨uE⟩ …
Showing the 12 most recent of 19 on this concept.
- KEAM 2026Set eng-2026-04174 marksMCQQ.The CORRECT statement among the following regarding electromagnetic waves is (A) They can travel through vacuum (B) They consist of only electric field (C) They consist of only magnetic field (D) They require a medium to propagate (E) They move with a velocity of 3×108 cms−1
›Reveal solutionSolution
EM waves propagate through vacuum, carrying mutually perpendicular oscillating electric and magnetic fields at speed c.
Examining the options:
- (A) True — a changing electric field creates a magnetic field and vice versa, so the wave is self-sustaining and needs no material medium (sunlight reaching Earth through space proves it).
- (B) False — it has both fields, not just electric. …
- KEAM 2026Set eng-2026-04184 marksMCQQ.A radio can tune in to any station in the 7.5 MHz to 12 MHz band. The corresponding wavelength band is (A) 75m-12m (B) 22.5m-36m (C) 40m-25m (D) 20m-45m (E) 15m-24m
›Reveal solutionSolution
Using λ=c/f, the 7.5 MHz end maps to 40 m and the 12 MHz end to 25 m, giving a band of 40m–25m.
λ=fc,c=3×108ms−1
For f=7.5MHz=7.5×106Hz:
λ=7.5×1063×108=40m
For f=12MHz=12×106Hz: …
- KEAM 2026Set eng-2026-04204 marksMCQQ.If the total energy transferred to a completely absorbing surface by an EM wave in unit time is 3.6 J, then the radiation pressure exerted by the wave on the surface is (A) 1×108Nm−2 (B) 1.8×108Nm−2 (C) 1×107Nm−2 (D) 1.2×107Nm−2 (E) 1.2×10−8Nm−2
›Reveal solutionSolution
For a completely absorbing surface the momentum delivered per unit time is cU/t.
For an electromagnetic wave completely absorbed by a surface, the force (rate of momentum transfer) equals the power divided by the speed of light. With energy delivered per unit time tU=3.6 J s−1: …
- KEAM 2026Set eng-2026-04214 marksMCQQ.Microwaves are (A) used in radio and television communications (B) having frequency range from 54 MHz to 890 MHz (C) short wavelength radio waves (D) produced by hot bodies and molecules (E) absorbed by ordinary glass
›Reveal solutionSolution
Microwaves = short-wavelength radio waves.
Microwaves occupy wavelengths of about 1,mm to 0.3,m (frequencies ∼109–1011,Hz), i.e. the short-wavelength end of the radio band, generated by devices such as klystrons and magnetrons. Options describing radio/TV frequency ran …
- KEAM 2026Set eng-2026-04224 marksMCQQ.In a plane electromagnetic wave if the amplitude of oscillating electric field is 45 Vm−1 then the amplitude of the oscillating magnetic field is (A) 2.5×10−8 T (B) 1.5×10−7 T (C) 3×10−8 T (D) 1.5×10−8 T (E) 2.5×10−7 T
›Reveal solutionSolution
In an EM wave the field amplitudes satisfy B0=E0/c. …
- KEAM 2026Set pha-2026-0418F4 marksMCQQ.Identify the two electromagnetic waves A and B having respective wavelengths 2 cm and 580 nm (A) A is microwave and B is visible light (B) A is infrared and B is ultraviolet ray (C) A is radio wave and B is visible light (D) A is infrared and B is visible light (E) A is radio wave and B ultraviolet ray
›Reveal solutionSolution
λ=2cm is microwave, λ=580nm is visible light. …
- KEAM 2026Set pha-2026-0420F4 marksMCQQ.If an EM wave travels in a medium with εr=4, μr=1, its speed (in ms−1) in terms of c (c = velocity of light in free space) is (A) c (B) 2c (C) 2c (D) 3c (E) 4c
›Reveal solutionSolution
v=c/εrμr=c/4⋅1=c/2.
The speed of an electromagnetic wave in a medium is
v=εrμrc.
With εr=4 and μr=1: …
- KEAM 2025Set eng-2025-04234 marksMCQQ.When a ray of light moves from one medium to another medium, (A) its frequency remains unchanged (B) its frequency alone changes (C) its wavelength remains unchanged (D) both its frequency and wavelength change (E) its velocity remains constant
›Reveal solutionSolution
When light passes into another medium its frequency stays unchanged.
Concept and Intuition
Frequency is fixed by the source and is conserved across a boundary (the fields must oscillate continuously at the interface). Speed and wavelength change with the medium's refractive index, but frequency does not.
Step-by-Step Solution
- v = f*lambda; on entering a new medium v changes.
- f is set by the source and is conserved at the boundary. …
- KEAM 2025Set eng-2025-04264 marksMCQQ.An electromagnetic wave travelling in vacuum has its electric field component, E=15sin[1.57y+5.4t]j^. The wavelength of the wave is (A) 4.0 m (B) 3.0 m (C) 2.5 m (D) 2.0 m (E) 1.0 m
›Reveal solutionSolution
The propagation constant is k=1.57 m−1, giving wavelength λ=2π/k=4.0 m.
The wave is E=15sin(1.57y+5.4t)j^, of the form E=E0sin(ky+ωt).
The angular wavenumber is k=1.57 m−1=λ2π. …
- KEAM 2025Set eng-2025-04274 marksMCQQ.The speed of electromagnetic waves in a medium depends on the (A) intensity of the wave (B) initial phase of the wave (C) permittivity and permeability of the medium (D) energy it carries (E) reflectivity of the medium
›Reveal solutionSolution
Electromagnetic wave speed is fixed by the medium's electric and magnetic properties: v=με1.
From Maxwell's equations, the speed of an electromagnetic wave in a medium is determined solely by its permittivity ε and permeability μ:
v=με1. …
- KEAM 2025Set pha-2025-0424F4 marksMCQQ.In a plane electromagnetic wave, the magnetic field is given by B=400×10−6sin[(4.0×10−4)(t−x/c)] T. The peak value of electric field (in Vm−1) is (A) 8×104 (B) 6×104 (C) 4×104 (D) 3×104 (E) 12×104
›Reveal solutionSolution
In an EM wave E0=cB0=3×108×400×10−6=12×104 V m−1.
In a plane electromagnetic wave the peak electric and magnetic fields are related by
E0=cB0.
Here the amplitude of the magnetic field is B0=400×10−6T, so …
- KEAM 2025Set pha-2025-0429F4 marksMCQQ.If the frequency of an electromagnetic wave is 2 MHz, then the time period of oscillation of the accelerated charge is (A) 2.5×10−7s (B) 1×10−7s (C) 5×10−7s (D) 6×10−7s (E) 2×10−7s
›Reveal solutionSolution
The oscillation period equals the reciprocal of the frequency: T=1/(2×106Hz)=5×10−7s.
The accelerated charge oscillates at the same frequency as the electromagnetic wave it radiates. With f=2MHz=2×106Hz, …
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