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Exercises · 8.8

Q.Suppose that the electric field amplitude of an electromagnetic wave is E0=120 N/CE_0 = 120\ \text{N/C} and that its frequency is ν=50.0 MHz\nu = 50.0\ \text{MHz}.

(a) Determine, B0B_0, ω\omega, kk, and λ\lambda.
(b) Find expressions for E\mathbf{E} and B\mathbf{B}.
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For an electromagnetic wave in vacuum, the magnetic amplitude is B0=E0/cB_0 = E_0 / c, the angular frequency is ω=2πν\omega = 2\pi\nu, the wave number is k=ω/ck = \omega / c, and the wavelength is λ=c/ν\lambda = c / \nu. Here B0=4.00×10−7 TB_0 = 4.00 \times 10^{-7}\ \text{T}, ω=3.14×108 rad/s\omega = 3.14 \times 10^8\ \text{rad/s}, k=1.05 rad/mk = 1.05\ \text{rad/m}, λ=6.00 m\lambda = 6.00\ \text{m}, and the wave travels along xx with E\mathbf{E} along yy and B\mathbf{B} along zz.


The core idea is that in an electromagnetic wave, the electric and magnetic fields are intimately linked through Maxwell’s equations. In free space, the wave speed is c=3.00×108 m/sc = 3.00 \times 10^8\ \text{m/s}, and the amplitudes satisfy E0=cB0E_0 = c B_0. The frequency ν\nu tells us how fast the fields oscillate, and from it we get the angular frequency ω=2πν\omega = 2\pi\nu. The wavelength λ\lambda follows from λ=c/ν\lambda = c / \nu, and the wave number k=2π/λk = 2\pi / \lambda. Once we have these parameters, we can write the full expressions for E\mathbf{E} and B\mathbf{B} as sinusoidal waves, choosing a direction of propagation (say +x+x) and mutually perpendicular polarization directions.

Let’s work through each part.

  1. Magnetic amplitude B0B_0 The relation between the peak electric and magnetic fields in vacuum is E0=cB0E_0 = c B_0. So

B0=E0c=120 N/C3.00×108 m/s=4.00×10−7 T.B_0 = \frac{E_0}{c} = \frac{120\ \text{N/C}}{3.00 \times 10^8\ \text{m/s}} = 4.00 \times 10^{-7}\ \text{T}.

This is a very small field — typical for radio waves.

  1. Angular frequency ω\omega ω=2πν\omega = 2\pi \nu. With ν=50.0 MHz=50.0×106 Hz\nu = 50.0\ \text{MHz} = 50.0 \times 10^6\ \text{Hz},

ω=2π(50.0×106)=3.14×108 rad/s.\omega = 2\pi (50.0 \times 10^6) = 3.14 \times 10^8\ \text{rad/s}.

(Using π≈3.14\pi \approx 3.14.)

  1. Wavelength λ\lambda For any wave, λ=c/ν\lambda = c / \nu.

λ=3.00×10850.0×106=6.00 m.\lambda = \frac{3.00 \times 10^8}{50.0 \times 10^6} = 6.00\ \text{m}.

This is in the radio band — about the length of a car.

  1. Wave number kk k=2π/λk = 2\pi / \lambda, so

k=2π6.00=1.05 rad/m.k = \frac{2\pi}{6.00} = 1.05\ \text{rad/m}.

Alternatively, k=ω/ck = \omega / c gives the same: 3.14×108/3.00×108=1.05 rad/m3.14 \times 10^8 / 3.00 \times 10^8 = 1.05\ \text{rad/m}.

Tip

You can always check consistency: kλ=2πk \lambda = 2\pi and ω=kc\omega = k c must hold. Here 1.05×6.00=6.30≈2π1.05 \times 6.00 = 6.30 \approx 2\pi, good enough.

Now for part (b): we need expressions for E\mathbf{E} and B\mathbf{B}. We must choose a direction of propagation and orientations for the fields. The standard choice: let the wave travel along the +x+x axis. Then E\mathbf{E} and B\mathbf{B} are perpendicular to each other and to the direction of propagation. A common convention is to take E\mathbf{E} along the yy-axis and B\mathbf{B} along the zz-axis. The wave is sinusoidal, so we write:

E(x,t)=E0sin⁡(kx−ωt) j^,\mathbf{E}(x,t) = E_0 \sin(kx - \omega t)\,\hat{\mathbf{j}},

B(x,t)=B0sin⁡(kx−ωt) k^.\mathbf{B}(x,t) = B_0 \sin(kx - \omega t)\,\hat{\mathbf{k}}. …

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