Modulation. Definition One signal (carrier) varies according to the changes in another signal (modulator) Either amplitude modulation (AM) or frequency.

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Presentation transcript:

Modulation

Definition One signal (carrier) varies according to the changes in another signal (modulator) Either amplitude modulation (AM) or frequency modulation (FM).

Amplitude Modulation Type #1 balanced/ring/double-sideband suppressed carrier amplitude modulation f 1 (t) * f 2 (t)

a f -f a t timefrequency a t f -f a f a a t carrier modulator result

f c - f m f c f c + f m carrier sin(2  f c  t) modulator sin(2  f m  t) f a sidebands sum and difference frequencies

Amplitude Modulation Type #2 double-sideband amplitude modulation 0.5 * (1.0 + f 1 (t)) * f 2 (t) f 1 is offset to range between 0.0 and 1.0

a f -f a t timefrequency a t f -f a f a a t carrier modulator result

f c - f m f c f c + f m f a 0.5 * (1.0 + M f 1 (t)) * f 2 (t) alternatively, where M is the modulation index At 100% modulation, that is, M = 1.0,

Overmodulation occurs when M > 1.0 the f 1 part ranges below zero and greater than 1.0 a t If [0.5 * (1.0 + M f 1 (t))] < 0.0, then replace with 0.0. carrier modulator

Amplitude Modulation Type #3 single-sideband, suppressed carrier amplitude modulation Pretty hard to do digitally!

Frequency Modulation f inst = f c  + F dv * sin(2  f m  t) amp * sin(2  f inst  t) where f c is the carrier frequency, f m is the modulator frequency and f inst is the instantaneous frequency

Frequency Modulation f inst = f c  + F dv * sin(2  f m  t) f t F dv fcfc instantaneous frequency

Frequency Modulation Index M = F dv / f m F dv = f m * M f inst = f c  + f m * M * sin(2  f m  t) amp * sin(2  f inst  t)

f c -3f m f c -2f m f c -f m f c f c +f m f c +2f m f c +3f m f a J 0 (M) J 1 (M) J 2 (M) J 3 (M) -J 1 (M) J 2 (M) -J 3 (M) Sidebands at ( f c  +/- n f m) Amplitudes at J n (M) where J n is a Bessel function of the nth order n=0 --- carrier n=1 --- first sideband pair etc.

Bessel Functions

f a J0J0 J1J1 J2J2 J3J3 -J 1 J2J2 -J 3 Folding Around 0 Hz -J 0 -J 1 -J 2 +J 3 +J 1 -J 2 +J 3 Components appear to fold around zero with reversed sign

f a +J 0 J1J1 J2J2 J3J3 -J 1 J2J2 -J 3 Chowning FM J4J4 J4J4 f a -J 1 J 0 - J 2 J 1 + J 3 J 2 - J 4 J 3 + J 5 J 4 - J 6 C:M 1:1

t M Chowning FM Trumpet C:M 1:1 Amplitude envelope shape also serves to control the frequency modulation index

f a C:M Ratios J 0 + J 1 J 1 - J 2 J 2 + J 3 f a J0J0 J1J1 J1J1 -J 2 J2J2 1 : 2 1 : 3 Every Mth harmonic is missing.

a C:M Ratios f J0J0 J1J1 J3J3 f a -J 1 J2J2 -J 3 J2J2 J0J0 J1J1 J2J2 J1J J2J2 J3J3 3 : 1 1 : inharmonic partials

t M Chowning FM Clarinet 0.1 C:M 3 : 2 Amplitude envelope must be separated from the frequency modulation index t a

f a -J 1 - J 2 J0J0 J1J1 Energy starts in the 3rd harmonic. Every 2nd harmonic is missing. Chowning FM Clarinet C:M 3 : 2 J2J2

t M Chowning FM Percussion C:M 1: t a M = 25: wood drum; 10: bell; 2 drum 1.0 drum bell wood drum

f a Detuning produces beats at 2* X FM detuning 1 : 1 +/- X Hz 1000 :

Extensions to FM: Multiple carriers + carrier 1carrier 2 modulator

f a Multiple Carriers formants f c1 f c2 voice synthesis

Extensions to FM: Complex Modulating Wave + modulator 1modulator 2 carrier +

Multiple Modulator Sidebands Multiple Modulator FM produces sidebands at f c +/- i f m1 +/- k f m2 like one FM pair is modulated by the other (f c +/- i f m1 ) +/- k f m2

Multiple Modulator Sidebands Example C: M1 : M2 1 : 1: 4 M 1 = 1, M 2 = 0.2 All cross combinations are formed 1:11:4 J J J J 3.02 Spreads energy out and limits the influence of dynamic M

Example: String Synthesis 1 : 1 : 3 : 4 Each M dependent on frequency 5-6 Hz Vibrato Hz random fluctuations Attack noise: 20% to 0% in.2 sec M +1 for.2 sec Detuning 1.5 to 4 Hz