Approximate a plane E&M wave with this large sum....

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SUMMARY

This discussion focuses on approximating a plane electromagnetic (E&M) wave using a large sum of electric polarization vectors defined by P(z,t) = pcos(kz-ωt). The setup involves an infinite line along the z-axis with polarization in the x-direction, uniformly distributed in space and in phase. The participants debate the feasibility of this construction to accurately represent the electric and magnetic fields of a plane E&M wave, with one contributor clarifying the concept of polarization being perpendicular to the line.

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Spinnor
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I would like to approximate a plane electromagnetic wave with a very large sum of the following.

Let an infinite line, say the z axis, have a electric polarization on that line and perpendicular to that line, say the x direction to be specific given by,

P(z,t) = pcos(kz-ωt). The polarization is a function of both space and time. Now let there be a uniform density of such lines in all space all parallel to one another, all in phase, and with them all polarized in the x direction. Will such a construction approximate the electric and magnetic fields of plane E&M wave?

Thanks!
 
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Spinnor said:
I would like to approximate a plane electromagnetic wave with a very large sum of the following.

Let an infinite line, say the z axis, have a electric polarization on that line and perpendicular to that line, say the x direction to be specific given by,

P(z,t) = pcos(kz-ωt). The polarization is a function of both space and time. Now let there be a uniform density of such lines in all space all parallel to one another, all in phase, and with them all polarized in the x direction. Will such a construction approximate the electric and magnetic fields of plane E&M wave?

Thanks!
I just cannot understand the question. How can we have polarisation on that line and also perpendicular to it?
 
tech99 said:
I just cannot understand the question. How can we have polarisation on that line and also perpendicular to it?

Just imagine at each point of the line a polarization vector that is also perpendicular to the line. Polarization is charge times a distance, just imagine the distance is very small, as small as you wish with charge increased so that distance times charge is a constant. Let the distance be of order the string length in string theory, that is pretty damn small.

Sorry for the confusion.
 

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