Doubts on Exercise Wording: Energy Density & Poynting Vector

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SUMMARY

The discussion centers on the calculation of mean energy density and the Poynting vector in electromagnetic theory. The energy density is defined as ##u=\varepsilon_0 (cB)^2##, with the mean energy density calculated as ##=\frac{1}{2}\varepsilon_0 (cB)^2##, considering the averaging over ##cos^2 (\omega t)##. Additionally, the mean amplitude of the Poynting vector is expressed as ##=\frac{B^2 c}{\mu_0}##, emphasizing the importance of using the RMS magnetic field for accurate calculations. The discussion concludes that the average energy density can be derived directly from the RMS value without further averaging.

PREREQUISITES
  • Understanding of electromagnetic theory, specifically energy density and Poynting vector concepts.
  • Familiarity with the equations for energy density and Poynting vector in electromagnetism.
  • Knowledge of RMS (Root Mean Square) calculations in the context of magnetic fields.
  • Basic proficiency in mathematical averaging techniques, particularly for trigonometric functions.
NEXT STEPS
  • Study the derivation of the Poynting vector in electromagnetic waves.
  • Learn about RMS calculations for varying waveforms in electromagnetic fields.
  • Explore the implications of averaging techniques in energy density calculations.
  • Investigate the relationship between electric and magnetic fields in wave propagation.
USEFUL FOR

This discussion is beneficial for physics students, educators, and professionals in electromagnetism, particularly those focused on energy density calculations and the Poynting vector in electromagnetic theory.

lorenz0
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Homework Statement
In a certain place on Earth, the magnitude of the magnetic field of solar radiation is equal to ##B##.
Calculate the average energy density of solar radiation in that area and the amplitude of the Poynting vector.
Relevant Equations
##u=\varepsilon_0 (cB)^2##, ##S=\frac{B^2 c}{\mu_0}##
I have doubts about the wording of the exercise:

(1) energy density is ##u=\varepsilon_0 (cB)^2## but since the question asks for mean energy density should I perhaps average over ##cos^2 (\omega t)## (there due to the ##B^2##) and thus use ##<u>=\frac{1}{2}\varepsilon_0 (cB)^2##?

(2) it seems to me that usually, due to the rapid changing of the electric and magnetic fields, one is interested in the mean of the amplitude of the Poynting vector ##<S>=\frac{B^2 c}{\mu_0}##, so perhaps that is the one I should compute (even if the text doesn't say so)?

I would be grateful for your feedback.
 
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I presume the magnetic field quoted is the RMS field. This is the only meaningful term to use because the wave shape of the radiation is not known, being noise-like.
Therefore I think the average energy density may be calculated direct from that value without further averaging.
 
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