Finding the average energy density of an EM wave in a magnetic field

In summary: If so, then you would use the following equation to find the fraction of the wave that passes through the polariser:frac(2c2B02ε0)
  • #1
Matt S
2
0
Hi, I've not posted on here before but I'm trying to keep on top of work over the summer and I'm having some real problems with this question

Homework Statement



Consider the plane polarised EM wave in a source free vacuum with magnetic field B = (1,1,0)B0cos(kz-wt) where B0 = 0.001T. Find the direction of propagation of the wave, the average energy density of the wave and the fraction of this energy which would pass through a perfect polaroid sheet at normal incidence if the angle between B and the transmission axis of the polariser is 30o.

Homework Equations



For the second part, I'm pretty sure you have to use U=B2/u0 where U is the energy density and u0 is the permeability of free space.

The Attempt at a Solution


The first part seems relatively simple, the wave travels perpendicularly to the magnetic field, so it moves in the (0,0,1) direction.

The second part asks for the average energy density but since B varies with respect to both time and position I'm not sure how to find it, would I have to integrate the expression for B with respect to t and then use the equation for U?

Obviously without an answer to part two I can't complete the third section. However, I'm pretty sure I have to find the fraction of the wave that passes through the polariser and hence find its energy density and then express that as a fraction of the incident energy density. I'm quite new to polarisation so I don't really know where to start and looking online has just confused me so far. Suggestions or links to relevant material would be really appreciated.

Thanks a lot.
 
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  • #2
The E field and B field are perpendicular, and both of these are perpendicular to the direction of propagation of the wave. If you can find the E field expression, the Poynting vector (cross product of E and B) will give you the direction of propagation and the energy flux. The gradient of the Poynting vector will give you the energy density.

As far as the polarizer part, I'm pretty sure when they give you transmission axis, that's referring to the electric field and not the magnetic field. So again you need to find which way the E field points and go from there.
 
  • #3
Okay, so I used the relationship E=cB to find that the electric field acts in the (1,-1,0) direction and hence that the wave does indeed propagate in the (0,0,1) direction. I then used U=ε0E2 to find that the energy density is U=2c2B02ε0

I'm still confused about the polariser, did you mean that the angle between the magnetic field and electric field is 30o?
 
Last edited:

1. What is the formula for finding the average energy density of an EM wave in a magnetic field?

The formula for finding the average energy density of an EM wave in a magnetic field is given by U = (B2)/(2μ0), where U represents the energy density, B is the magnetic field strength, and μ0 is the permeability of free space.

2. How is the energy density of an EM wave related to its magnetic field?

The energy density of an EM wave is directly proportional to the square of the magnetic field strength. This means that as the magnetic field strength increases, the energy density also increases.

3. What is the unit of measurement for the average energy density of an EM wave in a magnetic field?

The unit of measurement for the average energy density of an EM wave in a magnetic field is joules per cubic meter (J/m3).

4. Can the average energy density of an EM wave in a magnetic field ever be negative?

No, the average energy density of an EM wave in a magnetic field can never be negative. It is always a positive value, representing the amount of energy present in a given volume of space.

5. How can the average energy density of an EM wave in a magnetic field be used in practical applications?

The average energy density of an EM wave in a magnetic field can be used to calculate the amount of energy that can be extracted from the wave for practical purposes. It is also used in the design and optimization of various devices that utilize electromagnetic energy, such as antennas and transformers.

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