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Poynting Vector: a Plane EM Wave in 3D

A light wave is a braid of two fields: an electric field and a magnetic field, oscillating at right angles to each other and to the direction the wave travels. Their cross product, the Poynting vector S = E x B, points the way the energy flows and measures how much. For a wave travelling forward, E and B rise and fall together, so S is always positive: energy is carried steadily in one direction, never backward, even though the fields themselves keep flipping sign. Averaged over a cycle it settles to half the peak, which is exactly the intensity your eye or a solar panel feels. Twist the polarization into a circle and the fields trace helices of constant length, so the flow is perfectly smooth. Trap the wave between mirrors into a standing wave and something striking happens: E and B fall out of step, the Poynting vector sloshes back and forth, and the net energy transport drops to zero. The scene shows the E and B fields propagating with the energy-flow arrows; the diagnostic plots the three quantities and the time-averaged flow.

Figure 1. A plane electromagnetic wave and its Poynting vector. Top: the electric field E (red) and magnetic field B (blue) at right angles, propagating along z, with the energy-flow S = E x B arrows (gold). Bottom: the E and B components and the Poynting flow S along the wave, with the cycle-averaged flow (dashed). Method: closed-form plane-wave fields, S = E x B with c = 1.
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WHAT TO TRY

  • Watch the linear wave: E and B peak together, and the gold energy-flow arrows stay forward, never reversing.
  • Read the lower plot: the Poynting curve never dips below zero, and its dashed average sits at half the peak, the intensity.
  • Switch to circular polarization: E and B trace constant-length helices and the energy flow is perfectly steady.
  • Switch to a standing wave: E and B fall out of step, the Poynting flow sloshes both ways, and its average drops to zero.