Verified Solution • 2025–26 Session moderate

QJEEM24Ph333b: JEE Main 2024 Physics - Class 12 JEEM24Ph333b Solution: The electric field in an electromagnetic wave is given by . The …

The electric field in an electromagnetic wave is given by E→=i^40cos⁡ω(t−z/c)NC−1\overrightarrow{\mathrm{E}}=\hat{i} 40 \cos \omega(\mathrm{t}-z / \mathrm{c}) \mathrm{NC}^{-1} . The magnetic field induction of this wave is (in SI unit) :

Multiple Choice Options

  • A B→=j^40ccos⁡ω(t−z/c)\overrightarrow{\mathrm{B}}=\hat{j} \frac{40}{\mathrm{c}} \cos \omega(\mathrm{t}-z / \mathrm{c})
  • B B→=i^40ccos⁡ω(t−z/c)\overrightarrow{\mathrm{B}}=\hat{i} \frac{40}{\mathrm{c}} \cos \omega(\mathrm{t}-z / \mathrm{c})
  • C B⃗=j^40cos⁡ω(t−z/c)\vec{B}=\hat{j} 40 \cos \omega(t-z / c)
  • D B→=k^40ccos⁡ω(t−z/c)\overrightarrow{\mathrm{B}}=\hat{k} \frac{40}{\mathrm{c}} \cos \omega(\mathrm{t}-z / \mathrm{c})

Step-by-Step Verified Solution

To determine the magnetic field induction of the given electromagnetic wave, we need to use the relationship between the electric field E→\overrightarrow{\mathrm{E}} and the magnetic field B→\overrightarrow{\mathrm{B}} in an electromagnetic wave. For an electromagnetic wave propagating in vacuum, the following relation holds:

B→=E→×k^c\overrightarrow{\mathrm{B}} = \frac{\overrightarrow{\mathrm{E}} \times \hat{\mathrm{k}}}{\mathrm{c}}

where:

  • E→\overrightarrow{\mathrm{E}} is the electric field.
  • k^\hat{\mathrm{k}} is the unit vector in the direction of propagation of the wave.
  • c\mathrm{c} is the speed of light in a vacuum.

Given the electric field:

E→=i^40cos⁡ω(t−z/c)NC−1\overrightarrow{\mathrm{E}}=\hat{i} 40 \cos \omega(\mathrm{t}-z / \mathrm{c}) \mathrm{NC}^{-1}

The wave is propagating in the zz -direction, so k^=z^\hat{\mathrm{k}} = \hat{z} . The unit vector i^\hat{\mathrm{i}} represents the xx -direction.

The magnetic field induction is given by:

B→=(i^40cos⁡ω(t−z/c))×z^c\overrightarrow{\mathrm{B}} = \frac{(\hat{\mathrm{i}} 40 \cos \omega(\mathrm{t}-z / \mathrm{c})) \times \hat{\mathrm{z}}}{\mathrm{c}}

The cross product i^×z^\hat{\mathrm{i}} \times \hat{\mathrm{z}} yields j^\hat{\mathrm{j}} (the unit vector in the yy -direction):

B→=j^40cos⁡ω(t−z/c)c\overrightarrow{\mathrm{B}} = \hat{\mathrm{j}} \frac{40 \cos \omega(\mathrm{t}-z / \mathrm{c})}{\mathrm{c}}

Therefore, the magnetic field induction is:

B→=j^40ccos⁡ω(t−z/c)\overrightarrow{\mathrm{B}}=\hat{\mathrm{j}} \frac{40}{\mathrm{c}} \cos \omega(\mathrm{t}-z/\mathrm{c})

The correct answer is:

Option A:

B→=j^40ccos⁡ω(t−z/c)\overrightarrow{\mathrm{B}}=\hat{j} \frac{40}{\mathrm{c}} \cos \omega(\mathrm{t}-z / \mathrm{c})

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