Beating with signals of different amplitude

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Discussion Overview

The discussion revolves around the behavior of signals formed by the addition of two sinusoids with different amplitudes and frequencies. Participants explore the mathematical representation of these signals, particularly focusing on the concept of beat frequencies and envelopes, and the potential for deriving a formula similar to known identities for equal amplitudes.

Discussion Character

  • Exploratory
  • Mathematical reasoning
  • Technical explanation

Main Points Raised

  • One participant notes the known result for equal amplitude sinusoids and seeks to understand the case for differing amplitudes, proposing a formula that includes terms for amplitude variation.
  • Another participant suggests using complex exponentials to clarify the manipulation of the signals, leading to a focus on the real part of the resulting expression.
  • A participant expresses difficulty in manipulating the expression into the desired form and seeks assistance.
  • Discussion includes a method for rewriting the expression as a product of sum and difference terms, leading to a more complex formula that captures the behavior of the signals.
  • Further algebraic manipulation yields a formula that includes a beat envelope and a cosine term, with participants discussing the implications of the arctangent term in the expression.
  • Some participants propose approximations for small terms in the context of slightly different frequencies, while others caution against simplifying the expression too much.
  • A later reply raises the question of whether the derived formulas can be generalized to functions of time, suggesting a potential application in digital signal processing.

Areas of Agreement / Disagreement

Participants generally agree on the mathematical approaches and manipulations discussed, but there is no consensus on the necessity or appropriateness of approximating certain terms. The discussion remains unresolved regarding the implications of the arctangent term and its behavior under different conditions.

Contextual Notes

Participants express uncertainty about the effects of varying amplitudes and the implications of approximations made in the derivations. The discussion includes unresolved mathematical steps and assumptions regarding the relationships between the terms involved.

odiakkoh
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Okay: here's the question:

It's a well-known thing that when you add two sinusoids of equal amplitude and different frequency then you end up with a signal with the mean of the frequencies and a beat envelope. This just comes from the trig identity:

[tex]\cos(a) + \cos(b) = 2\cos(\frac{a+b}{2}) \cos(\frac{a-b}{2})[/tex]

Now... here's the tricky bit: what happens if the two signals have different amplitudes?

I can get some kind of intuitive feel for what would happen by considering the limit of one signal being much stronger than the other, but I'd really like to be able to find some formula, similar to the above, perhaps with a form similar to this:

[tex]A\cos(a) + B\cos(b) = (A+B)\cos(x)(1-z\cos(y))[/tex]

where x is the signal frequency, y is the beat frequency, and z is some number determining by how much the signal amplitude varies due to the beats.

Or perhaps this isn't possible? Anyhow: does anyone have any ideas?
 
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If you write it in terms of complex exponentials,

[tex]Ae^{i\omega_1t}+Be^{i\omega_2t} = Ae^{i\omega_1t}\left(1+\frac{B}{A}e^{i(\omega_2-\omega_1)t}\right)[/tex]

which might make it a little clearer.
 
Thanks... So now we're left with the problem of taking the real part of the RHS, i.e. evaluating this:

[tex]\Re\left( Ae^{iat}\left(1+\frac{A}{B}e^{i(b-a)t}\right)\right)[/tex]

I've had a go, but I just can't manage to manipulate the result into the form I want.
 
You don't need to take the real part, actually. You can draw all the necessary conclusions from the formula as it is. In particular, remember

[tex]\left|e^{i\theta}\right|=1[/tex]

So from that information, then, what conclusions can you draw by looking at the envelope term?
 
odiakkoh said:
Okay: here's the question:

It's a well-known thing that when you add two sinusoids of equal amplitude and different frequency then you end up with a signal with the mean of the frequencies and a beat envelope. This just comes from the trig identity:

[tex]\cos(a) + \cos(b) = 2\cos(\frac{a+b}{2}) \cos(\frac{a-b}{2})[/tex]

Now... here's the tricky bit: what happens if the two signals have different amplitudes?

I can get some kind of intuitive feel for what would happen by considering the limit of one signal being much stronger than the other, but I'd really like to be able to find some formula, similar to the above, perhaps with a form similar to this:

[tex]A\cos(a) + B\cos(b) = (A+B)\cos(x)(1-z\cos(y))[/tex]

where x is the signal frequency, y is the beat frequency, and z is some number determining by how much the signal amplitude varies due to the beats.

Or perhaps this isn't possible? Anyhow: does anyone have any ideas?

There is a trick in rewriting the expression:
[tex]f=Acos(a)+Bcos(b)[/tex]
as a product of the sum and difference of the two terms given.
First write the given expression as:
[tex]f=Acos\left(\frac{a+b+a-b}{2}\right)+Bcos\left(\frac{b+a+b-a}{2}\right)[/tex]
Then you need to expand it, and recollect the terms, giving:
[tex]f=\left(A+B\right)cos\left(\frac{a+b}{2}\right)cos\left(\frac{a-b}{2}\right)-\left(A-B\right)sin\left(\frac{a+b}{2}\right)sin\left(\frac{a-b}{2}\right)[/tex]

In case A and B are equal, you get the expression you've already mentioned. In case these are not equal, the second term comes in the picture.
 
Thanks, coomast, that's exactly the kind of expression I was looking for. Neat trick, too!
 
After further algebra

Taking this a little further, I've managed to rearrange this into an even more revealing form. The formula looks a little bulky to start, but please bear with me...

[tex]\left[A^2+B^2 + 2AB\cos\left(a-b\right)\right]^{1/2} \cos\left[\frac{a+b}{2} + \arctan\left(\frac{A-B}{A+B}\tan\left(\frac{a-b}{2}\right)\right)\right][/tex]

The term in the left square brackets is the beat envelope, oscillating slowly with frequency (a-b). I'm happy with that bit. The cosine term to the right of it is the signal, oscillating close to the (a+b)/2 frequency... but the tan and arctan parts on the right kind of ruin it as its not obvious at all what effect they have.

Can anyone think of a clever way of rewriting the arctangent term? It may be neccesary to make some approximation here. Perhaps A>>B or B<<A could be useful.
 
Nice way of taking it a bit further :-) I forgot about this method. Anyway, why would you rearrange the arctan? It is (in case of slightly different frequencies) a small term. Approximating this could be done by considering for small x:

[tex]tan(x)\approx x[/tex]

and

[tex]arctan(x)\approx x-\frac{x^3}{3}[/tex]

This is however something you need to investigate. Are all terms small or not? In my opinion I would leave the formula as it is. It is in fact the solution to the original question. Besides, it's far too nice to be approximated :-)
 


odiakkoh said:
Taking this a little further, I've managed to rearrange this into an even more revealing form. The formula looks a little bulky to start, but please bear with me...

[tex]\left[A^2+B^2 + 2AB\cos\left(a-b\right)\right]^{1/2} \cos\left[\frac{a+b}{2} + \arctan\left(\frac{A-B}{A+B}\tan\left(\frac{a-b}{2}\right)\right)\right][/tex]

The term in the left square brackets is the beat envelope, oscillating slowly with frequency (a-b). I'm happy with that bit. The cosine term to the right of it is the signal, oscillating close to the (a+b)/2 frequency... but the tan and arctan parts on the right kind of ruin it as its not obvious at all what effect they have.

Can anyone think of a clever way of rewriting the arctangent term? It may be neccesary to make some approximation here. Perhaps A>>B or B<<A could be useful.

Absolutely brilliant derivation!
I'd really be interested how did you get all this done. A pointer to a book would suffice, no need to type the whole thing. The reason I'm asking is: I'm dealing with same functions, with only difference being that [tex]a,b,A,B[/tex] are all functions (we could say polynomials) of x. I'm more comfortable talking in terms of time, cause I'm into digital signal processing, but just as well. Could I just switch constants A,B with A(t),B(t)?

For the previous eq:
[tex] A\cos(a) + B\cos(b) = (A+B)\cos(x)(1-z\cos(y))[/tex]
it is trivial to see that A,B can be swapped with functions A(t),B(t), so it's looking good so far. However I'm not sure if all the magic you did, that results in that aractan etc is also "immune" to such a swap.
Please let me know if you can. I'm googleing like crazy with no luck so far.

Thank you in any case!
Sash
 
  • #10


odiakkoh said:
Taking this a little further, I've managed to rearrange this into an even more revealing form. The formula looks a little bulky to start, but please bear with me...

[tex]\left[A^2+B^2 + 2AB\cos\left(a-b\right)\right]^{1/2} \cos\left[\frac{a+b}{2} + \arctan\left(\frac{A-B}{A+B}\tan\left(\frac{a-b}{2}\right)\right)\right][/tex]

The term in the left square brackets is the beat envelope, oscillating slowly with frequency (a-b). I'm happy with that bit. The cosine term to the right of it is the signal, oscillating close to the (a+b)/2 frequency... but the tan and arctan parts on the right kind of ruin it as its not obvious at all what effect they have.

Can anyone think of a clever way of rewriting the arctangent term? It may be neccesary to make some approximation here. Perhaps A>>B or B<<A could be useful.

Absolutely brilliant derivation!
I'd really be interested how did you get all this done. A pointer to a book would suffice, no need to type the whole thing. The reason I'm asking is: I'm dealing with same functions, with only difference being that [tex]a,b,A,B[/tex] are all functions (we could say polynomials) of x. I'm more comfortable talking in terms of time, cause I'm into digital signal processing, but just as well. Could I just switch constants A,B with A(t),B(t)?

For the previous eq:
[tex] A\cos(a) + B\cos(b) = (A+B)\cos(x)(1-z\cos(y))[/tex]
it is trivial to see that A,B can be swapped with functions A(t),B(t), so it's looking good so far. However I'm not sure if all the magic you did, that results in that arctan etc is also "immune" to such a swap.
Please let me know if you can. I'm googleing like crazy with no luck so far.

Thank you in any case!
Sash
 

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