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---- /!\ '''Edit conflict - other version:''' ----
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---- /!\ '''Edit conflict - your version:''' ----
Suppose you have unmodulated sinusoidal signal, '''e^w t^'''

This signal has the phase of
 . '''phi(t) = w t,'''
and frequency of
 . '''f(t) = 1/(2 pi) * dphi/dt = w/(2 pi) = f0.'''

---- /!\ '''End of edit conflict''' ----
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 . f(t) = f0 + df Cos(2 pi fm t)
 . phi(t) = Integrate[f(t) dt] = w t + df/fm * Sin(2 pi fm t)
 . '''f(t) = f0 + df Cos(2 pi fm t)'''
 . '''phi(t) = Integrate[f(t) dt] = w t + df/fm * Sin(2 pi fm t)'''
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This indicates that the modulation depth of FM is given by m = df / fm. This indicates that the modulation depth of FM is given by '''m = df / fm'''.

Frequency modulation and phase modulation are physically equivalent.


/!\ Edit conflict - other version:


Suppose you have unmodulated sinusoidal signal, ew t

This signal has the phase of phi(t) = w t, and frequency of f(t) = 1/(2 pi) * dphi/dt = w/(2 pi) = f0.


/!\ Edit conflict - your version:


Suppose you have unmodulated sinusoidal signal, ew t

This signal has the phase of

  • phi(t) = w t,

and frequency of

  • f(t) = 1/(2 pi) * dphi/dt = w/(2 pi) = f0.


/!\ End of edit conflict


Now we apply the frequency modulation with frequency deviation of df and modulation frequency of fm:

  • f(t) = f0 + df Cos(2 pi fm t)

  • phi(t) = Integrate[f(t) dt] = w t + df/fm * Sin(2 pi fm t)

Now think about the phase modulation with modulation depth of m and modulation frequency of fm:

This means that the effect of FM is the same as that of PM. This indicates that the modulation depth of FM is given by m = df / fm. For given df, FM gives a larger modulation depth with a lower modulation frequency.

FMandPM (last edited 2012-01-03 23:02:40 by localhost)