P-State Lightwave: Angular Frequency & Amplitude

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The discussion focuses on deriving the expression for a P-state lightwave with specified angular frequency and amplitude, propagating at a 45° angle in the xy-plane. Participants clarify the components of the electric field, suggesting that the wave should indeed propagate in the z-direction, with the correct representation involving both x and y components. The wavenumber vector is discussed, emphasizing its relation to the wavelength and direction of propagation, leading to the conclusion that the wave can be expressed as E(z,t)=Eo Cos(kz-wt). There is some confusion about the correct axis representation and whether components for the j and k vectors are necessary. Overall, the conversation highlights the complexities of wave propagation and the mathematical expressions involved.
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Here's the question that I've tried working it out...but sort of blocked at some places:

Write an expression for a P-state lightwave of angular frequency w and amplitude Eo propagating along a line in the xy-plane at 45° to the x-axis and having its plane of vibration corresponding to the xy-plane. At t=0, y=0, and x=0 the field is zero.

And this is what I've done so far...so if anyone can help me out here or tell me if I'm going to the right direction that'll be great.

i got: Eoy = Eo cos45°; Eox=Eo sin45° (in here, I'm not sure if i put the right axis or it's supposed to be Eoy and Eoz)
E(x,t) = Eo cos(kx-wt+1/4π) (once again, i don't know if it's E(x,t) and i assumed that there's no component for the j and k vector)?

kinda lost :blushing:
 
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i think the wave should be propagating in the z direction if it's propagating at 45 degrees to the x-axis, it's also at 45 degrees to the y-axis.

So, i think you're looking for something more like

E(z,t)=Eo Cos(kz-wt) or something..

i've got an exam in the subject in a weeks time and I'm a little lost too :-)
 
The wavenumber is a vector related to the wavelength and corresponds to the direction of propagation so in your case

\vec k = \frac {2\pi}{\lambda} \frac {\hat i + \hat j}{\sqrt 2} = \frac {\omega}{c} \frac {\hat i + \hat j}{\sqrt 2}

where the latter expression holds only in vacuum so your wave will have components containing sines and cosines of the phase \vec k \cdot \vec x - \omega t.
 
How do you get the sqrt(2)? (nvmd its probably from the new unit vector)
 
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