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Angle Modulation Time-varying frequency Introduction to angle modulation Relationship between FM and PM FM bandwidth

AngleModulation - Stanford UniversityInstantaneousFrequency In principle, frequency of a signal at an instant in time depends on entire signal (Hilbert transform) For generalized sinusoids,

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Page 1: AngleModulation - Stanford UniversityInstantaneousFrequency In principle, frequency of a signal at an instant in time depends on entire signal (Hilbert transform) For generalized sinusoids,

Angle Modulation

◮ Time-varying frequency

◮ Introduction to angle modulation

◮ Relationship between FM and PM

◮ FM bandwidth

Page 2: AngleModulation - Stanford UniversityInstantaneousFrequency In principle, frequency of a signal at an instant in time depends on entire signal (Hilbert transform) For generalized sinusoids,

Spectrogram

This spectrogram shows a whistler in the VLF band.

Page 3: AngleModulation - Stanford UniversityInstantaneousFrequency In principle, frequency of a signal at an instant in time depends on entire signal (Hilbert transform) For generalized sinusoids,

Spectrum Analyzer

Page 4: AngleModulation - Stanford UniversityInstantaneousFrequency In principle, frequency of a signal at an instant in time depends on entire signal (Hilbert transform) For generalized sinusoids,

Spectrum Analyzer (cont.)

Page 5: AngleModulation - Stanford UniversityInstantaneousFrequency In principle, frequency of a signal at an instant in time depends on entire signal (Hilbert transform) For generalized sinusoids,

Graphic Equalizer

Page 6: AngleModulation - Stanford UniversityInstantaneousFrequency In principle, frequency of a signal at an instant in time depends on entire signal (Hilbert transform) For generalized sinusoids,

Instantaneous Frequency

◮ In principle, frequency of a signal at an instant in time depends on entiresignal (Hilbert transform)

◮ For generalized sinusoids, we can use a simpler approach. Suppose

ϕ(t) = A cos θ(t) .

Then θ(t) is the generalized angle. For a true sinusoid,

θ(t) = ωct+ θ0 .

This is linear with slope ωc and offset θ0

◮ The generalized angle is not limited to [0, 2π]. Wrapping introducesdiscontinuities.

◮ Matlab has unwrap function to remove discontinuities.

Page 7: AngleModulation - Stanford UniversityInstantaneousFrequency In principle, frequency of a signal at an instant in time depends on entire signal (Hilbert transform) For generalized sinusoids,

Instantaneous Frequency (cont.)

◮ Instananeous frequency is derivative of generalized angle:

ωi(t) =dθ

dt= θ′(t)

◮ By Fundamental Theorem of Calculus,

θ(t) =

∫ t

−∞

ωi(u) du = θ(0) +

∫ t

0

ωi(u) du

◮ We can modulate a generalized sinusoid by using a signal m(t) to varyeither θ(t) or ωi(t).

◮ In either case, the frequency of the modulated signal changes as afunction of m(t).

Page 8: AngleModulation - Stanford UniversityInstantaneousFrequency In principle, frequency of a signal at an instant in time depends on entire signal (Hilbert transform) For generalized sinusoids,

Instantaneous Frequency (cont.)

Page 9: AngleModulation - Stanford UniversityInstantaneousFrequency In principle, frequency of a signal at an instant in time depends on entire signal (Hilbert transform) For generalized sinusoids,

Phase Modulation (PM) & Frequency Modulation (FM)

◮ In PM, phase is varied linearly with m(t):

θ(t) = ωct+ kpm(t) ⇒ ϕPM(t) = cos(

ωct+ kpm(t))

The instantaneous frequency is

ωi(t) =dθ

dt= ωc + kpm(t)

If m(t) varies rapidly, then the frequency deviations are larger.

◮ In FM, frequency deviation is linear in m(t):

ωi(t) = ωc + kfm(t)

The angle is

θ(t) =

∫ t

−∞

(

ωc + kfm(t))

du = ωct+ kf

∫ t

−∞

m(u) du

Page 10: AngleModulation - Stanford UniversityInstantaneousFrequency In principle, frequency of a signal at an instant in time depends on entire signal (Hilbert transform) For generalized sinusoids,

Relationship Between FM and PM

◮ Phase modulation of m(t) = frequency modulation of m(t).

◮ Frequency modulation of m(t) = phase modulation of∫

m(u) du.

Page 11: AngleModulation - Stanford UniversityInstantaneousFrequency In principle, frequency of a signal at an instant in time depends on entire signal (Hilbert transform) For generalized sinusoids,

Generalized Angle Modulation

◮ We can vary phase using a linear transform of message signal:

ϕEM(t) = A cos(

ωct+ h(t) ∗m(t))

= A cos

(

ωct+

∫ t

−∞

m(u)h(t − u) du

)

We assume that impulse response h(t) is causal.

◮ PM (h(t) = kpδ(t)) and FM (h(t) = kfu(t)) are special cases.

◮ We recover m(t) from phase by using inverse filter H−1(s).

E.g., for FM the inverse of integration is differention.

Page 12: AngleModulation - Stanford UniversityInstantaneousFrequency In principle, frequency of a signal at an instant in time depends on entire signal (Hilbert transform) For generalized sinusoids,

FM Example: fc = 100 MHz, kf = 2π × 105

Instantaneous frequency:

fi = fc +kf2π

m(t) = 108 + 105m(t)

fi,min = 99.9 MHz

fi,max = 100.1 MHz

Is the modulated signal confined to the frequency band 99.9− − 10.1+ ?

No! The bandwidth is approximately 300 KHz.

Page 13: AngleModulation - Stanford UniversityInstantaneousFrequency In principle, frequency of a signal at an instant in time depends on entire signal (Hilbert transform) For generalized sinusoids,

PM Example: fc = 100 MHz, kp = 10π

Instantaneous frequency:

fi = fc +kp2π

m(t) = 108 + 5m(t)

fi,min = 99.9 MHz

fi,max = 100.1 MHz

FM modulation by m(t) is same as PM modulation by m(t).

Page 14: AngleModulation - Stanford UniversityInstantaneousFrequency In principle, frequency of a signal at an instant in time depends on entire signal (Hilbert transform) For generalized sinusoids,

Frequency Shift Keying (FSK)

The binary message can be detected using two filters tuned for the twofrequencies.

FSK is a historically important digital modulation scheme. The Bell 103modem used frequencies 1070 and 1270 for originating station.

Page 15: AngleModulation - Stanford UniversityInstantaneousFrequency In principle, frequency of a signal at an instant in time depends on entire signal (Hilbert transform) For generalized sinusoids,

Phase Shift Keying (PSK)

The binary message can be detected by correlating with sinusoids of a fixedfrequency but different phases.

The sinusoids are 180◦ out of phase but synchronized with the carrier.

Page 16: AngleModulation - Stanford UniversityInstantaneousFrequency In principle, frequency of a signal at an instant in time depends on entire signal (Hilbert transform) For generalized sinusoids,

PSK: Direct Modulation

If kp = π/2 and m(t) takes on only values +1 and −1, then

ϕFM(t) = A cos(

ωct+ kpm(t))

= A cos(

ωct+π

2m(t)

)

=

{

A sinωct when m(t) = −1

−A sinωct when m(t) = 1

The figure on the previous slide corresponds to bit duration 7/fc, wherefc is the carrier frequency.

Phase changes of ±π are possible at the end of each bit period.The transmitter must low pass filter the PSK signal.