Chapter 3: Problem 4
Imagine an electromagnetic wave with its \(\overrightarrow{\mathrm{E}}\) -field in the \(y-\) direction. Show that Eq. (3.27) $$ \frac{\partial E}{\partial x}=-\frac{\partial B}{\partial t} $$ applied to the harmonic wave \(\overrightarrow{\mathbf{B}}\) $$ \overrightarrow{\mathbf{E}}=\overrightarrow{\mathbf{E}}_{0} \cos (k x-\omega t) \quad \overrightarrow{\mathbf{B}}=\overrightarrow{\mathbf{B}}_{0} \cos (k x-\omega t) $$ yields the fact that $$ E_{0}=c B_{0} $$ in agreement with Eq. (3.30)
Short Answer
Step by step solution
Understand the Setup
Calculate \( \frac{\partial E}{\partial x} \)
Calculate \( \frac{\partial B}{\partial t} \)
Apply \( \frac{\partial E}{\partial x} = -\frac{\partial B}{\partial t} \)
Simplify to Find \( E_0 = c B_0 \)
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Key Concepts
These are the key concepts you need to understand to accurately answer the question.
Maxwell's Equations
- Gauss's Law: This law states that the electric flux through a closed surface is proportional to the charge enclosed by the surface. It can be expressed as \( abla \cdot \mathbf{E} = \frac{\rho}{\epsilon_0} \).
- Gauss's Law for Magnetism: This states that the magnetic field \( \mathbf{B} \) has no divergence, meaning there are no magnetic monopoles. In mathematical terms, \( abla \cdot \mathbf{B} = 0 \).
- Faraday's Law of Induction: Describes how a time-varying magnetic field induces an electric field. It is given by \( abla \times \mathbf{E} = -\frac{\partial \mathbf{B}}{\partial t} \).
- Ampère's Law with Maxwell's Addition: Explains how magnetic fields are generated by electric currents and changing electric fields, expressed as \( abla \times \mathbf{B} = \mu_0 \mathbf{J} + \mu_0 \epsilon_0 \frac{\partial \mathbf{E}}{\partial t} \).
These equations lay the groundwork for understanding electromagnetic wave propagation, as they show that a changing electric field creates a magnetic field and vice versa.
Harmonic Waves
- For an electric field: \( \mathbf{E} = \mathbf{E}_0 \cos(kx - \omega t) \)
- For a magnetic field: \( \mathbf{B} = \mathbf{B}_0 \cos(kx - \omega t) \)
Where:
- \( \mathbf{E}_0 \) and \( \mathbf{B}_0 \) are the amplitudes of the electric and magnetic fields, respectively.
- \( k \) is the wave number, related to the wavelength as \( k = \frac{2\pi}{\lambda} \).
- \( \omega \) is the angular frequency, which is related to the period and frequency of the wave through \( \omega = 2\pi f \).
Harmonic waves are essential to understanding electromagnetic waves because they represent a simple form of wave propagation where electric and magnetic fields oscillate perpendicular to each other and the direction of travel.