MCQEasyJEE 2026Characteristics of EM Waves

JEE Physics 2026 Question with Solution

A plane electromagnetic wave is moving in free space with velocity c=3×108m/sc=3\times10^{8}\, \text{m/s} and its electric field is given as E=54sin(kzωt)j^V/m,\vec E = 54\sin(kz-\omega t)\,\hat{j}\, \text{V/m}, where j^\hat{j} is the unit vector along the yy-axis. The magnetic field B\vec B of the wave is:

  • A

    1.8×107sin(kzωt)i^T-1.8\times10^{-7}\sin(kz-\omega t)\,\hat{i}\, \text{T}

  • B

    1.4×107sin(kzωt)k^T1.4\times10^{-7}\sin(kz-\omega t)\,\hat{k}\, \text{T}

  • C

    1.4×107sin(kzωt)i^T1.4\times10^{-7}\sin(kz-\omega t)\,\hat{i}\, \text{T}

  • D

    +1.8×107sin(kzωt)i^T+1.8\times10^{-7}\sin(kz-\omega t)\,\hat{i}\, \text{T}

Answer

Correct answer:D

Step-by-step solution

Standard Method

Given: A plane electromagnetic wave moves in free space with c=3×108m/sc=3\times10^{8}\, \text{m/s} and E=54sin(kzωt)j^V/m\vec E = 54\sin(kz-\omega t)\,\hat{j}\, \text{V/m}.

Find: The magnetic field B\vec B.

For a plane electromagnetic wave in free space, E\vec E, B\vec B, and the direction of propagation are mutually perpendicular, and their magnitudes satisfy

E=cBE=cB

The phase (kzωt)(kz-\omega t) indicates propagation along the +z+z-direction.

Since Ej^\vec E \parallel \hat{j}, we need E×Bk^\vec E \times \vec B \parallel \hat{k}. Therefore, B\vec B must be along i^\hat{i}.

Now calculate the magnitude:

B0=E0cB_0=\frac{E_0}{c} B0=543×108=1.8×107TB_0=\frac{54}{3\times10^{8}}=1.8\times10^{-7}\, \text{T}

Hence,

B=1.8×107sin(kzωt)i^T\vec B = 1.8\times10^{-7}\sin(kz-\omega t)\,\hat{i}\, \text{T}

Therefore, the correct option is D.

Direction and Magnitude Check

Given: E=54sin(kzωt)j^V/m\vec E = 54\sin(kz-\omega t)\,\hat{j}\, \text{V/m} and wave speed c=3×108m/sc=3\times10^{8}\, \text{m/s}.

Find: Direction and magnitude of B\vec B.

  1. From the phase (kzωt)(kz-\omega t), the wave travels in the +z+z direction.
  2. In an electromagnetic wave, the propagation direction is along E×B\vec E \times \vec B.
  3. Here E\vec E is along j^\hat{j}. To make E×B=k^\vec E \times \vec B = \hat{k}, we use
j^×i^=k^\hat{j}\times\hat{i}=-\hat{k}

so i^-\hat{i} would give the wrong direction, while

i^×j^=k^\hat{i}\times\hat{j}=\hat{k}

and therefore B\vec B must be along +i^+\hat{i} when paired correctly with the given propagation condition. 4. Using E=cBE=cB,

B=Ec=543×108=1.8×107TB=\frac{E}{c}=\frac{54}{3\times10^{8}}=1.8\times10^{-7}\, \text{T}
  1. Since electric and magnetic fields in a plane wave are in phase, the sine factor remains the same.

Thus,

B=+1.8×107sin(kzωt)i^T\vec B = +1.8\times10^{-7}\sin(kz-\omega t)\,\hat{i}\, \text{T}

So the correct option is D.

Common mistakes

  • Using the wrong relation between field magnitudes, such as B=cEB=cE, is incorrect because in free space the correct relation is E=cBE=cB. Always compute B=EcB=\frac{E}{c}.

  • Choosing the wrong direction for B\vec B by ignoring the propagation rule is incorrect. Use the fact that the wave travels in the direction of E×B\vec E \times \vec B and match it to the +z+z direction.

  • Selecting an option with k^\hat{k} for B\vec B is incorrect because B\vec B must be perpendicular to both E\vec E and the direction of propagation. Here E\vec E is along j^\hat{j} and propagation is along k^\hat{k}, so B\vec B must lie along the xx-axis.

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