How to theoretically derive the sideband frequency values?

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The discussion focuses on deriving sideband frequency values from two combined signals, y1 and y2, represented as A cos(ω1t) and A cos(ω2t). It highlights that while the addition of these signals can illustrate beat frequencies, it does not generate sidebands, which arise from non-linear processes like modulation and mixing. The conversation references the need for a mathematical approach similar to that used for beat frequencies but acknowledges that simple addition does not yield the desired sideband frequencies. The participants emphasize the importance of understanding the distinction between adding and multiplying sinusoids in this context. Ultimately, the thread seeks clarification on how to properly derive sideband frequencies using trigonometric relations.
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Hi
If 2 signals of frequencies y1 = A cos ##\omega_1## t and y2 = A cos ##\omega_2## t are combined the resultant signal is given by y = y1 + y2
y = 2A cos (w1-w2)t/2 cos (w1+w2)t/2
If w1~w2 then one can plot the beat phenomenon from this equation.

But if w1 >> w2 as in the case of a carrier wave and a message wave. Then how can one get the sideband frequencies (w1-w2) and (w1+w2) from this ?

TIA
 
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bksree said:
Hi
If 2 signals of frequencies y1 = A cos ##\omega_1## t and y2 = A cos ##\omega_2## t are combined the resultant signal is given by y = y1 + y2
y = 2A cos (w1-w2)t/2 cos (w1+w2)t/2
If w1~w2 then one can plot the beat phenomenon from this equation.

But if w1 >> w2 as in the case of a carrier wave and a message wave. Then how can one get the sideband frequencies (w1-w2) and (w1+w2) from this ?

TIA
There is a difference between adding and multiplying two sinusoids. Which one are you asking about?

http://hyperphysics.phy-astr.gsu.edu/hbase/trid.html
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Sidebands are created with modulators and mixers which must be non-linear processes. The dominant operation is multiplication not addition. This is typically the second order term in a Taylor's expansion of the non-linear function, since higher order terms are smaller (i.e. less efficient). Addition does not create sum and difference frequencies.

Edit: Modulators are too broad of a category for this effect . Some modulators won't create sidebands, some will. Really it's mixers that do this.
 
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Hi
Thanks for your response.

I want to derive the relation to show the side band frequencies just like that obtained for the beat frequencies. And I want to do that using the simple trig relations you've shown.

I went through some oder posts and saw this (https://www.physicsforums.com/threads/sidebands-in-am-transmission.668449/) by 'sophiecentaur' where it is mentioned
But the easiest way to show how AM produces sidebands is to start with a formula which describes Amplitude Modulating a carrier wave with angular frequency ωc with a cosine modulating signal of frequency ωm does:
A =A0Cos(ωct)(1+Bcos(ωmt))

My waves are y1 = A1 cos ## \left( \omega_1 t \right)## and y2 = A2cos ## \left( \omega_2 t \right)##
Now, y1 + y2 = A1 cos ## \left( \omega_1 t \right)## + A2cos ## \left( \omega_2 t \right)##
= A1 cos(w1t) ( 1 + A2/A1 * cos(w2t)/cos(w1t) }
Now it looks like I am going off track!

Please help out

TIA
 
bksree said:
Hi
Thanks for your response.

I want to derive the relation to show the side band frequencies just like that obtained for the beat frequencies. And I want to do that using the simple trig relations you've shown.

I went through some oder posts and saw this (https://www.physicsforums.com/threads/sidebands-in-am-transmission.668449/) by 'sophiecentaur' where it is mentionedMy waves are y1 = A1 cos ## \left( \omega_1 t \right)## and y2 = A2cos ## \left( \omega_2 t \right)##
Now, y1 + y2 = A1 cos ## \left( \omega_1 t \right)## + A2cos ## \left( \omega_2 t \right)##
= A1 cos(w1t) ( 1 + A2/A1 * cos(w2t)/cos(w1t) }
Now it looks like I am going off track!
Please help out
TIA
Your equations are correct, but what are you trying to do?
Summing your two expressions y1 + y2 does NOT produce any sidebands, as you've been advised in previous posts.
 
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