Direction of polarization for monochromatic wave?

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Homework Help Overview

The problem involves determining the electric and magnetic field directions for a monochromatic plane wave with specified amplitude, frequency, and polarization. The wave travels towards a specific point in space, and the polarization is constrained to the xz plane.

Discussion Character

  • Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • Participants discuss the need to find unit vectors for the electric field and wave vector, questioning how to ensure these vectors meet the required conditions of unity and orthogonality.

Discussion Status

Some participants have pointed out the importance of ensuring the magnitude of the unit vector is one and that it must be perpendicular to the wave vector. There is ongoing exploration of the relationships between the components of the vectors and the conditions they must satisfy.

Contextual Notes

Participants note that the problem does not provide specific lengths for the components of the electric field vector, leading to uncertainty in how to derive the necessary unit vector. The discussion also highlights the requirement for the vectors to be orthogonal, which adds complexity to the problem.

magnesium12
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Homework Statement


Write down the (real) electric and magnetic fields for a monochromatic plane wave of amplitude Eo, frequency w, and phase angle zero traveling in the direction from the origin to the point (1,1,1) with polarization parallel to the xz plane.

I understand how to write the equations, I just don't understand how to get the correct direction for the electric and magnetic fields.

Homework Equations


## E(z,t) = E_o\cos(\hat k \cdot \hat r - \omega t) \hat n ##
## B(z,t) = \frac{E_o}{c}\cos(\hat k \cdot \hat r - \omega t) ( \hat k x \hat n) ##
## k = -\frac{\omega}{c} ##
## \hat n \cdot \hat k = 0 ##

The Attempt at a Solution


This is what I did:

## \hat n = \hat x + \hat z ##
## \hat k = \frac{\omega}{c} (\hat x + \hat y + \hat z) ##

So I thought that was all I was supposed to do to find the direction, but the solutions manual says these are the actual directions of n and k:

## \hat n =\frac { \hat x - \hat z}{\sqrt{2}} ##
## \hat k = \frac{\omega}{c} \frac{(\hat x + \hat y + \hat z)}{\sqrt{3}} ##

So where did those factors of sqrt(2) and sqrt(3) come from?
I appreciate any help!
 
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First, the question asks you to find the unit vector, so the magnitude of the vector which is supposed to be the answer should be unity. Second, you only know that ##\hat{n}## only has components along ##\hat{x}## and ##\hat{z}## but you are not given the length of each component, these are what you should calculate subject to the condition that the length of ##\hat{n}## is unity and that this vector is perpendicular to ##\hat{k}##.
 
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blue_leaf77 said:
First, the question asks you to find the unit vector, so the magnitude of the vector which is supposed to be the answer should be unity. Second, you only know that ##\hat{n}## only has components along ##\hat{x}## and ##\hat{z}## but you are not given the length of each component, these are what you should calculate subject to the condition that the length of ##\hat{n}## is unity and that this vector is perpendicular to ##\hat{k}##.

I don't think I understand.
So I would do
## n = \sqrt(a^2 + b^2)) = 1## Therefore: ##a^2= 1-b^2##
## k = \sqrt(c^2 + d^2 + e^2) = 1##
And then use this somehow:
## \hat n \cdot \hat k = nkcos\theta = 0##
## nkcos\theta = \sqrt((1-b^2) + b^2)\sqrt(c^2 + d^2 + e^2)cos\theta##
But since n = 1 and k =1, wouldn't that just leave me with nothing again?
 
If ##\mathbf{k}## is denoted such that it has components ##c##, ##d##, and ##e## then they must be known already since the problem tells you that ##\mathbf{k}## goes from the origin to the point (1,1,1). What you don't know yet are just ##a## and ##b##, i.e. two unknowns. You have figured out one equation relating these unknowns, which is
magnesium12 said:
## n = \sqrt(a^2 + b^2)) = 1## Therefore: ##a^2= 1-b^2##
.
The other equation you need is the orthogonality condition between ##\mathbf{k}## and ##\hat{n}##. To do this, it will be easier with component-by-component multiplication instead of the one like ##kn\cos \theta##.
 
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