Question:

The electric field of a plane electromagnetic wave is given by
\(\vec{E} = E_0\hat{i}\cos(kz)\cos(\omega t)\)
The corresponding magnetic field \(\vec{B}\) is then given by

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Use Faraday's law \(\nabla\times\vec{E} = -\frac{\partial\vec{B}}{\partial t}\) and integrate with respect to time.
Updated On: Nov 5, 2026
  • \(\vec{B} = \frac{E_0}{C}\hat{j}\sin(kz)\sin(\omega t)\)
  • \(\vec{B} = \frac{E_0}{C}\hat{j}\sin(kz)\cos(\omega t)\)
  • \(\vec{B} = \frac{E_0}{C}\hat{j}\cos(kz)\sin(\omega t)\)
  • \(\vec{B} = \frac{E_0}{C}\hat{k}\sin(kz)\cos(\omega t)\)
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The Correct Option is A

Solution and Explanation

\(\vec{E} = E_x\hat{i}\) depends on \(z\) and \(t\). \(\nabla\times\vec{E} = \frac{\partial E_x}{\partial z}\hat{j} = -E_0 k\sin(kz)\cos(\omega t)\,\hat{j}\).
Faraday: \(\frac{\partial\vec{B}}{\partial t} = -\nabla\times\vec{E} = E_0 k\sin(kz)\cos(\omega t)\,\hat{j}\).
Integrating over \(t\): \(\vec{B} = \frac{E_0 k}{\omega}\sin(kz)\sin(\omega t)\,\hat{j} = \frac{E_0}{c}\sin(kz)\sin(\omega t)\,\hat{j}\) (since \(\omega/k = c\)).
Answer: (1) \(\vec{B} = \frac{E_0}{C}\hat{j}\sin(kz)\sin(\omega t)\)
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