MCQEasyJEE 2024Characteristics of EM Waves

JEE Physics 2024 Question with Solution

The electric field of an electromagnetic wave in free space is represented as E=E0cos(ωtkx)i^E = E_0 \cos(\omega t - kx) \, \hat{i}. The corresponding magnetic induction vector will be:

  • A

    B=E0Ccos(ωtkx)j^B = E_0 C \cos(\omega t - kx) \, \hat{j}

  • B

    B=E0Ccos(ωtkx)j^B = \frac{E_0}{C} \cos(\omega t - kx) \, \hat{j}

  • C

    B=E0Ccos(ωt+kx)j^B = E_0 C \cos(\omega t + kx) \, \hat{j}

  • D

    B=E0Ccos(ωt+kx)j^B = \frac{E_0}{C} \cos(\omega t + kx) \, \hat{j}

Answer

Correct answer:B

Step-by-step solution

Standard Method

Given: The electric field is E=E0cos(ωtkx)i^\vec{E} = E_0 \cos(\omega t - kx) \, \hat{i}.

Find: The corresponding magnetic induction vector B\vec{B}.

For an electromagnetic wave in free space:

  • E\vec{E}, B\vec{B}, and the direction of propagation are mutually perpendicular.
  • The direction of propagation is given by E×B\vec{E} \times \vec{B}.
  • Their magnitudes satisfy
E=CBE = C B

so

B=ECB = \frac{E}{C}
  • Both fields are in the same phase.

From the phase term ωtkx\omega t - kx, the wave propagates along the positive xx-direction. Since E\vec{E} is along i^\hat{i}, the magnetic field must be perpendicular to both the propagation direction and E\vec{E}, and its magnitude must be E0C\frac{E_0}{C} with the same phase.

Thus,

B=E0Ccos(ωtkx)j^\vec{B} = \frac{E_0}{C} \cos(\omega t - kx) \, \hat{j}

Therefore, the correct option is B.

Direct EM Wave Relation

Given: E=E0cos(ωtkx)i^\vec{E} = E_0 \cos(\omega t - kx) \, \hat{i}

Find: B\vec{B}

Use the direct relation for an electromagnetic wave in free space:

B0=E0CB_0 = \frac{E_0}{C}

and E\vec{E} and B\vec{B} are in the same phase.

So the magnetic field must have the same cosine factor and amplitude E0C\frac{E_0}{C}. Hence,

B=E0Ccos(ωtkx)j^\vec{B} = \frac{E_0}{C} \cos(\omega t - kx) \, \hat{j}

Therefore, the correct option is B.

Common mistakes

  • Using B=E0CB = E_0 C instead of B=E0CB = \frac{E_0}{C} is incorrect because for electromagnetic waves in free space the relation is E=CBE = C B. Always divide the electric field amplitude by CC to get the magnetic field amplitude.

  • Changing the phase from ωtkx\omega t - kx to ωt+kx\omega t + kx is wrong because the electric and magnetic fields oscillate in the same phase. Keep the same phase factor in both fields.

  • Choosing a direction for B\vec{B} without checking the right-hand rule can lead to an inconsistent field orientation. Use the mutual perpendicularity of E\vec{E}, B\vec{B}, and the propagation direction, together with E×B\vec{E} \times \vec{B}.

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