A Questions about the energy of a wave as a Taylor series

AI Thread Summary
The discussion centers on the relationship between wave energy and amplitude, specifically how energy can be expressed through a Taylor series expansion. It highlights that energy is not strictly proportional to the square of the amplitude, as typically taught, but can include higher-order terms in the series. The participants question why energy does not depend on phase and why odd terms in the series are considered unimportant, linking this to the nature of sine and cosine functions. The conversation references Ben Crowell's insights on the topic, emphasizing the need for a clearer derivation of the Taylor series in this context. Overall, the thread seeks to clarify the mathematical foundations of wave energy in relation to amplitude.
Chump
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I've read that, in general, the energy of a wave, as opposed to what's commonly taught, isn't strictly related to the square of the amplitude. It can be seen to be related to a Taylor series, where E = ao + a1 A + a2A2 ... Also, that the energy doesn't depend on phase, so only even terms will occur and the Taylor series gets truncated to only be proportional to the amplitude squared.

My questions are:

  • Is there a derivation/more in-depth explanation of how the Taylor series came about for relating energy to amplitude?
  • Why doesn't energy depend on phase? (My guess is because it's based on a simple harmonic oscillator model)
  • Since phase isn't important, why will the odd terms in the series not be important? How are those two things related?
 
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Chump said:
I've read that, in general, the energy of a wave, as opposed to what's commonly taught, isn't strictly related to the square of the amplitude. It can be seen to be related to a Taylor series, where E = ao + a1 A + a2A2

Wait... what? How exactly is the energy of wave is due to "a Taylor series" and how does the Taylor series have anything to do with a description of a wave?

Where exactly did you get this idea?

Zz.
 
Then shouldn't you be asking this THERE? I don't understand why we at PF are the ones who have to clean up other people's mess.

Zz.
 
OK. First, I've asked this there already. It was pretty much the first thing I did. I could not get in touch with Ben Cromwell on the site. Also, no one else from that site gave an answer. Further, I could not get in touch with Ben via his outside site. I believe I've taken all of the proper channels, and I'd just like a little bit of insight from other avenues, if possible. You don't need to "clean up any mess." If you don't have any helpful insight, please move along because I didn't approach this in a disrespectful way. I'd appreciate it if no disrespect came my way. Thank you.
 
Chump said:
Since phase isn't important, why will the odd terms in the series not be important?
I am puzzled by that one too. @bcrowell knows his stuff, so I am pretty confident it is right, but it isn’t obvious to me either.
 
Chump said:
Is there a derivation/more in-depth explanation of how the Taylor series came about for relating energy to amplitude?
Ben is just saying that the energy E of the wave can be thought of as a function of its amplitude A, so we can expand this function E(A) in a Taylor series about A=0.
 
Dale said:
I am puzzled by that one too. @bcrowell knows his stuff, so I am pretty confident it is right, but it isn’t obvious to me either.
Nearest explanation I can come up with is...

Taylor series for a sin wave has odd powers...

Sin(X) = X1 - X3/3! + X5/5! -...

and a cos has even powers.

Cos(X) = 1 - X2/2! + X4/4! -...

Difference between cos and sin is phase.

But I'm not sure I believe that deleting one set or the other from a general series of both makes it ignore phase.

If your function is a sin wave and you delete the odd terms to remove phase what are you left with?
 
CWatters said:
Difference between cos and sin is phase.
That makes sense, but then why pick the cos instead of the sin. That seems like cos waves carry energy and sin waves don’t.

Edit: oh, that is even and odd powers of X not of A.
 
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