Question about the Poynting vector

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    Poynting vector Vector
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Discussion Overview

The discussion revolves around the Poynting vector in the context of monochromatic electromagnetic plane waves, focusing on its calculation and interpretation when using complex exponentials for the electric and magnetic fields. Participants explore the implications of these calculations on the behavior of the Poynting vector over time and space.

Discussion Character

  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • Some participants assert that the Poynting vector is given by the cross product of the electric and magnetic fields, \mathbf{S} = \mathbf{E} \times \mathbf{H}, rather than the product of their magnitudes.
  • There is a suggestion that the magnitude of the Poynting vector should be |\mathbf{S}| = \frac{E_0 B_0}{\mu_0}, but this is contested based on the time-varying nature of the fields.
  • Some participants propose that the Poynting vector is a vector field, as it varies with position along the wave propagation direction.
  • Concerns are raised about the constancy of the Poynting vector, with some arguing that it should not be constant due to points where the electric and magnetic fields are zero.
  • Others argue that the Poynting vector maintains a constant magnitude due to the constant phase relationship between the electric and magnetic fields in a plane wave.
  • A participant introduces the concept of a complex Poynting vector, suggesting that it should be expressed as \mathbf{S} = \frac{1}{2} \mathbf{E} \times \mathbf{H}^* when using complex amplitudes.

Areas of Agreement / Disagreement

Participants express multiple competing views regarding the behavior of the Poynting vector, particularly concerning its constancy and the interpretation of its magnitude. The discussion remains unresolved, with no consensus on the implications of using complex exponentials in the calculations.

Contextual Notes

Participants note that the use of complex exponentials may obscure the sinusoidal dependence of the fields on time and position, leading to confusion about the Poynting vector's behavior. There are also discussions about the definitions and interpretations of vector fields versus vectors in the context of electromagnetic waves.

fishh
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Suppose I have a monochromatic electromagnetic plane wave with the E-field linearly polarized in the x-direction (and the B-field linearly polarized in the y-direction). Then the Poynting vector should be pointing in the z direction with a magnitude equal to the product of the B and E-field magnitudes divided by the magnetic constant. But because they are complex, the magnitudes of the B and E field don't depend on time or position, which doesn't make sense, as the Poynting vector shouldn't be constant over all time. Of course, this can be solved by taking only the real parts of both solutions and multiplying them, but this would require breaking up the complex exponentials into cosines and sines. Is there anyway to do this without having to break up the complex exponentials?
 
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The Poynting vector is

\mathbf{S} = \mathbf{E}\times\mathbf{H}

not

\mathbf{S} \neq |\mathbf{E}|\times|\mathbf{H}|

If the fields vary in time, so does the Poynting vector.
 
Born2bwire said:
The Poynting vector is

\mathbf{S} = \mathbf{E}\times\mathbf{H}

not

\mathbf{S} \neq |\mathbf{E}|\times|\mathbf{H}|

If the fields vary in time, so does the Poynting vector.

Well that's true, but if I have an E-field like

E_0 \hat{x} e^{-i(kz -\omega t)}

And consequently, a B-field like

B_0 \hat{y} e^{-i(kz - \omega t)}

Then shouldn't the magnitude of the Poynting vector just be |\mathbf{S}| = |\mathbf{E}||\mathbf{H}| = \frac{E_0 B_0}{\mu_0}?
 
Last edited:
fishh said:
Well that's true, but if I have an E-field like

E_0 \hat{x} e^{-i(kz -\omega t)}

And consequently, a B-field like

B_0 \hat{y} e^{-i(kz - \omega t)}

Then shouldn't the magnitude of the Poynting vector just be |\mathbf{S}| = |\mathbf{E}||\mathbf{H}| = \frac{E_0 B_0}{\mu_0}?

In this case, yes.
 
Hi,

A small question concerning the calculation above.
When we take the expressions for E and B and evalute the cross product, the obtained result is a vector or a vector field ?

In other words, given a EM wave field it correct to say that the Poyinting Vector is also a vector field ?

Thank you in advance,

Best Regards,

DaTario
 
DaTario said:
Hi,

A small question concerning the calculation above.
When we take the expressions for E and B and evalute the cross product, the obtained result is a vector or a vector field ?

In other words, given a EM wave field it correct to say that the Poyinting Vector is also a vector field ?

Thank you in advance,

Best Regards,

DaTario

I think it is a vector field, as every z position has a different E and B field and thus, a different Poynting vector.

I'm not sure if the calculation I did was correct; a plane wave should not have a constant Poynting vector, as there are points where the E and B field are 0, and the magnitude of the Poynting vector should also be 0. I think there should be a sinusoidal dependence on z and t, but whenever I use complex exponentials, the dependence vanishes...
 
fishh said:
I think it is a vector field, as every z position has a different E and B field and thus, a different Poynting vector.

I'm not sure if the calculation I did was correct; a plane wave should not have a constant Poynting vector, as there are points where the E and B field are 0, and the magnitude of the Poynting vector should also be 0. I think there should be a sinusoidal dependence on z and t, but whenever I use complex exponentials, the dependence vanishes...

A plane wave has constant magnitude and the example you gave maintains a constant phase relationship between the two fields, so of course its Poynting vector also has constant magnitude.
 
Born2bwire said:
A plane wave has constant magnitude and the example you gave maintains a constant phase relationship between the two fields, so of course its Poynting vector also has constant magnitude.

The magnitude of the wave is only constant across planes perpendicular to the wave's motion. The magnitude of the E and B fields still vary sinusoidally with z (parallel planes with a different z component have a different magnitude), so shouldn't the magnitude of the Poynting vector change with z?
 
Maybe "amplitude" is a better word. Anyway, you are probably restricting your consideration to a particular instant in time. Think about what happens as time passes. There will be a particular maximum value for E and B at a given point, and, since you are talking about a plane wave, this value is the same for every point. The phase is an arbitrary choice that you make, and is no more physical than the location of z=0.
 
  • #10
Born2bwire said:
The Poynting vector is

\mathbf{S} = \mathbf{E}\times\mathbf{H}
...
When using the complex amplitudes, I believe that the expression should be

\mathbf{S}=\frac{1}{2}\mathbf{E}\times\mathbf{H}^*

This is the complex Poynting vector. The exponential factors that make the E and B fields a plane wave cancel out, due to the complex conjugation.
 

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