kkmans said:
I would like to ask which equation shows that wave energy is independent of frequency..?
Look in any first-year general physics textbook for the energy transmitted by any classical wave (string, sound, EM, etc).
ZapperZ said:
(section 8.2.2 in Griffiths 2nd Edition), you would have seen that the energy of a monochromatic plane wave is
[tex]U = \epsilon_0 E^2_0 cos^2(\kappa x - \omega t + \delta)[/tex]
This clearly has a frequency term. The confusion comes in when you are looking at the total energy [..] THEN you have integrated out the effects of frequency
Clearly this is the authoritive source (albeit a less developed version) so you should be able to find in the following paragraphs an expression for the intensity (likely represented as "I" rather than "U").
The first thing you should notice about the dependence you're giving is that it does not cause the "integrated" energy (over any period of time exceeding about a [itex]10^{-15}[/itex]th of a second) to increase with frequency, and this really should contradict what you have said. Moreover, if you cling to this definition, then you can never define a practical "energy per unit time" on any measurable scale.
ZapperZ said:
You're asking why, given a particular amplitude, the energy transmitted through a particular point by possible electromagnetic waves (with different frequencies) is not proportional to the internal energies of different stationary isolated mass-springs (in which the position of the mass
changes, but also with a particular amplitude, and the frequencies are equivalent with those of the EM waves)?
I really think I need you to explain what these two examples have in common. Then, why do you choose
increasing the spring stiffness to change frequency (which also increases energy) instead of just
decreasing the mass to change frequency (which does not change the energy)? Thirdly, how do you then derive from this the equivalent equation to in Griffiths?