Is there something as instanteneous intensity of a wave?

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The discussion centers on the concept of instantaneous intensity of electromagnetic waves, specifically questioning the definition of intensity as an average over one period of the wave. The formula for intensity is given as ##I=\frac{1}{dA} \frac{dE}{dt}##, indicating that intensity is time-dependent. The participant highlights that traditional texts define intensity using the average of ##c|A(t)|^{2}##, suggesting a practical approach rather than a strictly accurate one. The energy transport vector is defined as ##\vec{S}=\frac{1}{\mu_0}\vec{E}\times\vec{B}##, emphasizing the need to integrate this over an area for total energy transfer.

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At the moment I'm revising some interference and diffraction basics, and there is something that bothers me slightly and I can't quite figure it out.

The intensity of a wave over some area ##dA## is in general is ##I=\frac{1}{dA} \frac{dE}{dt}##. Clearly for an electromagnetic wave falling on a surface, the part ##\frac{dE}{dt}## is not constant and depends on time. So intensity should be a function of time.

In every text I encounter they seem to DEFINE the intensity as being the average over 1 period of ##c|A(t)|^{2}## where ##A## is the deviation of the wave at the area of interest. Are they simply using more practical definitions, and technically I'm correct above in a general sense OR am I missing something?
 
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The instantaneous rate of energy transport is going to be a function of the instantaneous electric and magnetic fields.

Here's a link with more:
http://hyperphysics.phy-astr.gsu.edu/hbase/waves/emwv.html

It gives the energy transport vector as

\vec{S}=\frac{1}{\mu_0}\vec{E}\times\vec{B} where \vec{E},\ \vec{B} are the electric and magnetic field vectors. Note that the direction of energy transport, being a cross product, is perpendicular to both, as one would expect.

By the way, that's the formula at a point. To get the energy transfer rate over an area, you'd need to integrate that formula over the area.
 

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