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An infinitely long solenoid, with its axis along \(\hat{k}\), carries a current I. In addition there is a uniform line charge density \(\lambda\) along the axis. If \(\vec{S}\) is the energy flux, in cylindrical coordinates \((\hat{\rho}, \hat{\phi}, \hat{k})\), then

  • A.\(\vec{S}\) is along \(\hat{\rho}\)
  • B.\(\vec{S}\) is along \(\hat{k}\)
  • C.\(\vec{S}\) has non zero components along \(\hat{\rho}\) and \(\hat{k}\)
  • D.\(\vec{S}\) is along \(\hat{\rho} \times \hat{k}\)

Answer: D

The energy flux \(\vec{S}\) is along \(\hat{\rho} \times \hat{k}\).

Inside the solenoid the magnetic field is axial, \(\vec{B} = \mu_{0} n I\hat{k}\). The line charge gives a radial electric field \(\vec{E} = \frac{\lambda}{2\pi\varepsilon_{0}\rho}\hat{\rho}\). The Poynting vector is

\[ \begin{aligned} \vec{S} &= \frac{1}{\mu_{0}}\vec{E} \times \vec{B} \\ &\propto \hat{\rho} \times \hat{k} = -\hat{\phi} \end{aligned} \]

so the energy flux circulates azimuthally. It has no \(\hat{\rho}\) or \(\hat{k}\) component, which rules out the other three options.

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