How Is Energy Flux Calculated in an Electromagnetic Wave?

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SUMMARY

The energy flux of an electromagnetic wave is calculated using the formula (1/2)ε0cE02, where ε0 is the permittivity of free space, c is the speed of light, and E0 is the peak electric field amplitude. This calculation accounts for the time-averaged power density, which is essential since the electric field E oscillates between 0 and E0. Misinterpretations can arise from assuming constant energy density, as the instantaneous power density is ε0cE2, which does not reflect the average over time.

PREREQUISITES
  • Understanding of electromagnetic wave properties
  • Familiarity with the concepts of energy density and power density
  • Knowledge of time-averaging in oscillatory systems
  • Basic grasp of the physics of light and electromagnetic theory
NEXT STEPS
  • Study the derivation of energy density in electromagnetic waves
  • Learn about the relationship between electric field amplitude and energy flux
  • Explore the concept of time-averaging in oscillatory motion
  • Review Walter Lewin's lectures on electromagnetic waves for clarity on terminology
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Students and professionals in physics, particularly those focusing on electromagnetism, electrical engineers, and educators seeking to clarify concepts related to energy flux in electromagnetic waves.

guillefix
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Hello,

The energy density of an electromagnetic wave is ε_{0}E^{2}. To calculate the energy flux, at least in the derivation's I've seen, people just multiply by the speed of the wave, i.e., c. But doesn't this assume that the energy density is constant at all points?; but E changes periodically! Why isn't it then the integral of the energy density in the corresponding volume, so it would give something close to a half of the usual answer i see!?

Thanks in advance
 
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Just read in here: http://hep.ph.liv.ac.uk/~hutchcroft/Phys258/CN6EMWaves.pdf that I was right yeah. Walter Lewin's lecture was a bit missleading.
 
Last edited by a moderator:
One has to be very careful with terminology and keep in mind exactly which quantity is being discussed. The instantaneous power density (W/m2) passing through a surface oriented perpendicular to the wave propagation direction is indeed ε0cE2.

However, the magnitude of E oscillates rapidly between 0 and the amplitude Emax (often called E0). Finding the time-average over a whole number of cycles gives half of the maximum power density, so the time-averaged power density (which is what we can actually measure in practice) is (1/2)ε0cEmax2 which is often written as (1/2)ε0cE02.

I haven't watched Levin's lecture so I don't know which terminology he's using.
 

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