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## Homework Statement

A harmonic EM-wave is propagating in glass in the +x-direction. The refractive index of the glass ##n = 1.4##. The wave number of the wave ##k = 30 \ rad/m##. The magnetic portion of the wave is parallel to the y-axis and its amplitude ##H_0 = 0.10A/m##. At ##t=0## and ##x = 0## the magnetic field vector ##\vec{H} = H_0 \hat{j} = +0.10A/m \ \hat{j}##.

a) Approximate the values for the permittivity (##\epsilon##) and permeability (##\mu##) of the type of glass in question.

b) Calculate the propagation speed, wavelength, angular frequency and frequency of the wave.

c) Calculate the amplitude of the electric field component of the wave at x=0, t=0 (remember to show the direction of the vector).

d) Write the expressions for the electric and magnetic field components in vector form.

## Homework Equations

Basic wave equation:

\begin{equation}

v = \lambda f

\end{equation}

The wave number:

\begin{equation}

k = \frac{\omega}{v} = \frac{2\pi f}{v}

\end{equation}

Relation between the magnetic and electric components of the wave resulting from them being in phase:

\begin{equation}

E = vB

\end{equation}

The definition of the refractive index:

\begin{equation}

n:= \frac{c}{v} \stackrel{Maxwell}{=} \frac{\sqrt{\epsilon \mu}}{\sqrt{\epsilon_0 \mu_0}}

\end{equation}

Total energy density of an EM-wave:

\begin{equation}

w = w_E + w_M = \frac{\epsilon E^2}{2} + \frac{\mu H^2}{2}

\end{equation}

As a result of ##E = vB##, the ratio of the energy densities of the electric and magnetic field components:

\begin{equation}

\frac{w_E}{w_M} = \mu \epsilon v^2 = 1

\end{equation}

## The Attempt at a Solution

**a)**I'm having trouble with this part. Looking at equations (4) and (6):

\begin{cases}

\epsilon \mu &= n^2 \epsilon_0 \mu_0\\

\epsilon \mu &= \frac{1}{v^2}

\end{cases}

This should be easily solvable, but my math head is not working(again). If I solve for either ##\epsilon## or ##\mu## in one equation and plug it into the other equation, it will cancel out and I'm only left with things that I already have values for. It seems I need more information. Not sure what.

**b)**Looking at equation (3) the velocity:

[tex]v = \frac{c}{n} = \frac{2.9979 \times 10^{8}m/s}{1.4} = 214 \ 135 \ 714.3 \ m/s[/tex]

Now from equation (1) the angular frequency:

\begin{array}{lll}

\omega

&= kv \\

&= (30rad/m)(214 \ 135 \ 714.3 \ m/s)\\

&= 6 \ 424 \ 071 \ 429 \ rad/s\\

&\approx 6.4 \ G \ rad/s

\end{array}

and frequency:

\begin{array}{lll}

f

&= \frac{\omega}{2 \pi}\\

&= \frac{6 \ 424 \ 071 \ 429 \ rad/s}{2\pi}\\

&= 1 \ 022 \ 422 \ 723 \ Hz\\

&\approx 1.0 \ GHz

\end{array}

Equation (1) gives us the wavelength:

\begin{array}{ll}

\lambda

&= \frac{c}{f}\\

&= \frac{214 \ 135 \ 714.3 \ m/s}{1 \ 022 \ 422 \ 723 \ Hz}\\

&= 0.2 \ 094 \ 395 \ 102 \ m\\

&\approx 0.21 \ m

\end{array}

**c)**From equation (3):

\begin{array}{ll}

E_0

&= vB_0\\

&= v \mu H_0

\end{array}

In need the value of ##\mu## for this (from part

**a**). The direction can be found out by using the right hand rule. If ##\hat{H}## is in the y-direction and the wave is propagating in the x-direction, the electric component must be in the z- direction. Since the waves are in phase, ##\hat{E}## must be in the +z-direction.(Right?)

**d)**Since the wave is harmonic, its components are sinusoidal. From

**c**we know the directions of the components, so we can write:

\begin{array}

\vec{E} = E_0 sin(\omega t - kx) \hat{k}\\

\vec{H} = H_0 sin(\omega t - kx) \hat{j}

\end{array}

And there you have it. All I really need help with is part

**a**. After that I should be able to solve for the electric field in part

**c**. I assume the rest of my answer is correct.

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