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An electromagnetic wave propagating in vacuum has electric and magnetic fields given by E(x,t)=E0cos(kxωt)\vec{E}(\vec{x}, t)=\vec{E}_0 \cos (\vec{k} \cdot \vec{x}-\omega t) and B(x,t)=B0cos(kxωt)\vec{B}(\vec{x}, t)=\vec{B}_0 \cos (\vec{k} \cdot \vec{x}-\omega t), where B0\vec{B}_0 is given by B0=k×E0/ω\vec{B}_0=\vec{k} \times \vec{E}_0 / \omega and the wave vector k\vec{k} is perpendicular to both E0\vec{E}_0 and B0\vec{B}_0. The magnitude of k\vec{k} and the angular frequency ω\omega satisfy the dispersion relation, ω/k=(μ0ϵ0)1/2\omega /|\vec{k}|=\left(\mu_0 \epsilon_0\right)^{-1 / 2}, where μ0\mu_0 and ϵ0\epsilon_0 are the permeability and permittivity of free space, respectively. Such a wave transports energy in both its electric and magnetic fields. Calculate the ratio of the energy densities of the magnetic and electric fields, uB/uEu_B / u_E, in this wave. Explain.

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We are given: -electric field in the propagating electromagnetic wave E(x,t)=E0cos(kxωt)\vec{E}(\vec{x},t)=\vec{E}_0\cdot \cos{(\vec{k}\cdot \vec{x}-\omega t)} -magnetic field in the propagating electromagnetic wave B(x,t)=B0cos(kxωt)\vec{B}(\vec{x},t)=\vec{B}_0\cdot \cos{(\vec{k}\cdot \vec{x}-\omega t)} -constant vector B0\vec{B}_0 is given by B0=(k×E0)/ω\vec{B}_0=(\vec{k} \times \vec{E}_{0})/\omega -dispersion relation that k\vec{k} and ω\omega satisfy: ω/k=(μ0ϵ0)1/2\omega/|\vec{k}|=(\mu_0 \cdot \epsilon_0)^{-1/2}

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