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A long straight wire, having radius \(a\) and resistance per unit length \(r\), carries a current \(I\). The magnitude and direction of the Poynting vector on the surface of the wire is

  • A.\(I^{2}r/2\pi a\), perpendicular to axis of the wire and pointing inwards
  • B.\(I^{2}r/2\pi a\), perpendicular to axis of the wire and pointing outwards
  • C.\(I^{2}r/\pi a\), perpendicular to axis of the wire and pointing inwards
  • D.\(I^{2}r/\pi a\), perpendicular to axis of the wire and pointing outwards

Answer: A

The Poynting vector has magnitude \(I^{2}r/2\pi a\), perpendicular to the axis and pointing inwards.

At the surface, the electric field driving the current is along the wire, \(E = Ir\) (the voltage drop per unit length), and the magnetic field circles the wire with \(H = I/(2\pi a)\). They are perpendicular, so

\[ S = EH = Ir \cdot \frac{I}{2\pi a} = \frac{I^{2}r}{2\pi a} \]

With \(\vec{E}\) along the current and \(\vec{H}\) circling it by the right-hand rule, \(\vec{E} \times \vec{H}\) points radially inward. This is the energy flowing in from the field to be dissipated as heat: multiplying by the surface area per unit length, \(2\pi a\), gives \(I^{2}r\), the Joule heating per unit length. An outward flux would have the wire supplying energy, and \(I^{2}r/\pi a\) would deliver twice the heat produced.

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