AM radio signal superimpostion/modulation

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SUMMARY

The discussion centers on the concept of wave superimposition in the context of Amplitude Modulation (AM) radio waves. Participants clarify that AM involves modulating the amplitude of a carrier wave in accordance with the instantaneous values of an audio signal. The equation Yam(t)=(Ac+As·cos(2πfst))·cos(2πfct) is introduced, where A represents amplitude, f is frequency, c denotes the carrier, and s signifies the signal. The discussion emphasizes that the resultant waveform is a complex representation of the carrier wave modulated by the audio signal.

PREREQUISITES
  • Understanding of Amplitude Modulation (AM) principles
  • Familiarity with wave superimposition concepts
  • Basic knowledge of Fourier's Theorem
  • Ability to interpret mathematical equations in signal processing
NEXT STEPS
  • Study the mathematical foundations of Amplitude Modulation
  • Explore Fourier's Theorem and its applications in signal analysis
  • Learn about the process of wave demodulation for AM signals
  • Investigate the differences between Amplitude Modulation and Frequency Modulation
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Students and professionals in electrical engineering, audio engineering, and telecommunications who are interested in understanding the principles of AM radio wave generation and modulation techniques.

sillyquark
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Homework Statement



Describe how the concept of wave superimposition is used to create AM radio waves.

Homework Equations





The Attempt at a Solution



O.K, I am not sure that I understand how this works. In the picture attached it shows the carrier frequency inside of the audio signal. The amplitude changes over time, so is the amplitude not proportional to the wavelength or frequency? If that is the case then would I be correct in saying that constructive/destructive wave interference is used to superimpose the amplitude of the carrier frequency to be similar with the audio signal's wavelength. Wave demodulation for AM signals measures the amplitude over time so that the wavelength can be known. With the wavelength and speed of light one can calculate the frequency of the audio signal, which is then amplified and converted into sound through the speakers.

Is this more or less correct?
 

Attachments

  • AM superimposition.png
    AM superimposition.png
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superimpose the amplitude of the carrier frequency to be similar with the audio signal's wavelength
Change the last word to "amplitude". AM is amplitude modulation, not frequency modulation. There is, of course a broadening of the frequency range from virtually a single carrier frequency to the range carrier - audioFreq to carrier + audioFreq, but you have not been asked about that.
 
So, superimposing the amplitude of the carrier frequency to be similar with the audio signal's amplitude/time gives us wavelength or frequency?
 
Dear sillyquark, AM wave is generated by modulating the carrier wave's amplitude proportional to the signal wave's instantaneous y offset from the x-axis (Suppose that you draw a standard Y-X coordinate to plot the signal wave), your attachment plot is an AM wave, with Both Side-Band
 
You didn't really answer my question, you just stated what the attachment displays.
 
sillyquark said:
You didn't really answer my question, you just stated what the attachment displays.

Sorry about that, I didn't get your idea just now.

I guess you're asking about this Y_{am}(t)=(A_c+A_s \cdot cos(2 \pi f_s t)) \cdot cos(2 \pi f_c t) ?

I'm not familiar with Latex in this forum, it took me so much time to adapt to it...
 
So, superimposing the amplitude of the carrier frequency to be similar with the audio signal's amplitude/time gives us wavelength or frequency?
It doesn't "give us wavelength or frequency". It gives the complex waveform at the bottom of your attachment picture. It has the carrier frequency waveform modulated in amplitude according to the audio signal.
 
O.K, I understand the concept but not thoroughly. Thanks for the help, this is all I should need for the answer. Genxium, what are the variables in the equation you posted?
 
sillyquark said:
O.K, I understand the concept but not thoroughly. Thanks for the help, this is all I should need for the answer. Genxium, what are the variables in the equation you posted?

A : Amplitude , f: frequency , c: carrier , s: signal.

and this is the simpliest example while the signal wave is a sinusoid wave, but according to Fourier's Theorem, any real wave could be regarded as a superposition of many sinusoid waves, this basic form is still useful in analysis
 
  • #10
Great, thanks, you've helped a lot.
 
  • #11
genxium said:
A : Amplitude , f: frequency , c: carrier , s: signal.

and this is the simpliest example while the signal wave is a sinusoid wave, but according to Fourier's Theorem, any real wave could be regarded as a superposition of many sinusoid waves, this basic form is still useful in analysis

And, in this case, a standard simple identity involving \cos A \cos B gives the superposition.
 

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