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Exercises · 8.6

Q.A charged particle oscillates about its mean equilibrium position with a frequency of 109 Hz10^{9}\ \text{Hz}. What is the frequency of the electromagnetic waves produced by the oscillator?

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An oscillating charge produces electromagnetic waves at the same frequency as its own oscillation. Since the charge oscillates at 109 Hz10^{9}\ \text{Hz}, the EM waves also have a frequency of 109 Hz10^{9}\ \text{Hz}.

The key idea here is beautifully simple: an oscillating electric charge is the source of electromagnetic waves, and the wave it produces cannot have a frequency different from the source's own motion. Let's see why.

When a charged particle (like an electron) moves back and forth, it creates a changing electric field. A changing electric field, by Maxwell's laws, generates a magnetic field, and a changing magnetic field regenerates an electric field — and so on. This self-sustaining chain propagates outward as an electromagnetic wave.

The crucial point: the source's oscillation drives the wave. The electric field at any point near the charge varies exactly as the charge's position varies. If the charge completes one full back-and-forth cycle in time TT, the electric field at a fixed point also completes one full cycle in the same TT. Therefore, the wave's frequency ff must equal the source's frequency f0f_0.

  1. Identify the source frequency. The problem states the charged particle oscillates with frequency f0=109 Hzf_0 = 10^{9}\ \text{Hz}.

  2. Relate source motion to wave production. The oscillating charge acts as an antenna. Its acceleration (since oscillation involves acceleration) produces electromagnetic radiation. The radiated field's time variation is locked to the source's motion — there is no mechanism for the wave to "wiggle" faster or slower than the charge itself.

  3. Apply the fundamental relation. For any electromagnetic wave produced by an oscillating dipole (which is what a single oscillating charge approximates), the wave frequency equals the oscillation frequency of the dipole. So: …

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