Which Direction Does the Electric Field Oscillate and the Wave Propagate?

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Homework Help Overview

The discussion revolves around determining the direction of oscillation of the electric field and the propagation direction of an electromagnetic wave in a vacuum, based on a given electric field expression.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants explore how to identify the direction of the electric field oscillation and the wave's propagation direction from the provided mathematical expression. Questions arise about the interpretation of the phase argument and the components of the wave vector.

Discussion Status

Some participants have provided insights into the relationship between the wave vector and the phase of the wave, while others have discussed how to approach the calculation of the associated magnetic field. There is an ongoing exploration of how to handle the components of the electric field in calculations.

Contextual Notes

Participants are navigating the complexities of electromagnetic wave properties and the mathematical representations involved, including the treatment of exponential terms in vector calculations.

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Homework Statement


Given the following EM wave propagating in vacuum, find the direction along which the electric field oscillates and the direction of propagation of the wave:

[tex]\vec{E} = (-3\hat{i} + 3\sqrt{3}\hat{j}) 10^4 e^{i[\frac{\pi}{3} (\sqrt{5}x + \sqrt{5/3} y10^7 - 8.1246 *10^{15} t]}[/tex]

Btw how can I prevent the thread template from reappearing every time I click preview post? It is quite annoying.

The Attempt at a Solution



I understand the electric field oscillates along the direction [itex]-1\hat{i} \sqrt{3}\hat{j}[/itex], by looking at the amplitide. But how do I determine the direction of propagation from the phase argument? Do I just treat the x and y in the phase as if they were unit vectors of [itex]\vec{k}[/itex]?
 
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Pretty much. You know a wave propagating in the k direction has a phase given by [itex]i(\vec{k}\cdot\vec{r}-\omega t)[/itex], so just pick out the components of k.
 
Thanks, I see it now. One more question, if I am asked to find the associated [itex]\vec{H}[/itex] field by calculating [itex]\frac{1}{\mu_0 c} \hat{u}\times \vec{E}[/itex], where û is the normalized wave vector, how would I split up the components of E for the determinant? Would it be like:[tex]E_x = -3\cdot10^4 e^{i[\frac{\pi}{3} (\sqrt{5}x + \sqrt{5/3} y10^7 - 8.1246 *10^{15} t]}[/tex][tex]E_y = 3\sqrt{3}\cdot10^4 e^{i[\frac{\pi}{3} (\sqrt{5}x + \sqrt{5/3} y10^7 - 8.1246 *10^{15} t]}[/tex]

for example? Or do I also have to split up the phase/exponent for each component of E?
 
You can keep the exponential part separate; it's part of the amplitude of the electric field. I would write the electric field as the product of a magnitude and a unit vector:
[tex]\vec{E} = \left(-\frac{1}{2}\hat{i}+\frac{\sqrt{3}}{2}\hat{j}\right)(3\times10^4~\mathrm{V/m})e^{i(\vec{k}\cdot\vec{r}-\omega t)}[/tex]The only part you need for the determinant is the unit vector. The rest just scales the result of the cross product.
 

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