Q.A plane electromagnetic wave of frequency travels in free space along the -direction. At a particular point in space and time, . What is at this point?
For an EM wave, and are perpendicular, in phase, and related by . Here .
The key idea is that in a plane electromagnetic wave, the electric and magnetic fields are not independent — they are linked by Maxwell’s equations. For a wave traveling in free space, the ratio of their magnitudes is fixed by the speed of light, and their directions are perpendicular to each other and to the direction of propagation.
The wave moves along the -direction. The electric field is given as , which points along the -axis. For the wave to travel along , the magnetic field must lie along the -axis — that’s the only remaining perpendicular direction. The sign (whether or ) is determined by the fact that must point in the direction of wave travel, which is .
Let’s work through it step by step.
- Recall the fundamental relation In free space, the magnitudes of and in an electromagnetic wave satisfy
where is the speed of light. This comes directly from Maxwell’s equations — the wave equation for and gives the same speed , and the fields are in phase with this ratio.
- Find the magnitude of Given , we have
- Determine the direction The wave travels along . The electric field is along . For the Poynting vector to point along , we need to be along . Using the right-hand rule: . So must be along .
A quick check: if you ever forget the cross product direction, use the cyclic order . Here is propagation, is , so must be — and the sign follows from .
- Write the final vector Therefore,
A common mistake is to forget that the frequency is irrelevant here — it only tells you the wave is in the radio band, but the relation holds for any frequency in free space. Don’t let extra data distract you.
The magnetic field at that point is .
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