Phase modulation (PM) is a modulation pattern for conditioning communication signals for transmission. It encodes a message signal as variations in the instantaneous phase of a carrier wave. Phase modulation is one of the two principal forms of angle modulation, together with frequency modulation.
In phase modulation,'' the instantaneous amplitude of the baseband signal modifies the phase of the carrier signal keeping its amplitude and frequency constant''
The phase of a carrier signal is modulated to follow the changing signal level (amplitude) of the message signal. The peak amplitude and the frequency of the carrier signal are maintained constant, but as the amplitude of the message signal changes, the phase of the carrier changes correspondingly.
Phase modulation is widely used for transmitting radio waves and is an integral part of many digital transmission coding schemes that underlie a wide range of technologies like Wi-Fi, GSM and satellite television.
PM is used for signal and waveform generation in digital synthesizers, such as the Yamaha DX7, to implement FM synthesis. A related type of sound synthesis called phase distortion is used in the Casio CZ synthesizers.

Theory

PM changes the phase angle of the complex envelope in direct proportion to the message signal. If ''m(t)'' is the message signal to be transmitted and the carrier onto which the signal is modulated is :$c(t)\; =\; A\_c\backslash sin\backslash left(\backslash omega\_\backslash mathrmt\; +\; \backslash phi\_\backslash mathrm\backslash right).$, then the modulated signal is :$y(t)\; =\; A\_c\backslash sin\backslash left(\backslash omega\_\backslash mathrmt\; +\; m(t)\; +\; \backslash phi\_\backslash mathrm\backslash right).$ This shows how $m(t)$ modulates the phase - the greater m(t) is at a point in time, the greater the phase shift of the modulated signal at that point. It can also be viewed as a change of the frequency of the carrier signal, and phase modulation can thus be considered a special case of FM in which the carrier frequency modulation is given by the time derivative of the phase modulation. The modulation signal could here be :$m(t)\; =\; \backslash cos\backslash left(\backslash omega\_\backslash mathrm\; t\; +\; h\backslash omega\_\backslash mathrm(t)\backslash right)\backslash $ The mathematics of the spectral behavior reveals that there are two regions of particular interest: *For small amplitude signals, PM is similar to amplitude modulation (AM) and exhibits its unfortunate doubling of baseband bandwidth and poor efficiency. *For a single large sinusoidal signal, PM is similar to FM, and its bandwidth is approximately ::$2\backslash left(h\; +\; 1\backslash right)f\_\backslash mathrm$, :where $f\_\backslash mathrm\; =\; \backslash omega\_\backslash mathrm/2\backslash pi$ and $h$ is the modulation index defined below. This is also known as Carson's Rule for PM.

Modulation index

As with other modulation indices, this quantity indicates by how much the modulated variable varies around its unmodulated level. It relates to the variations in the phase of the carrier signal: :$h\backslash ,\; =\; \backslash Delta\; \backslash theta\backslash ,$, where $\backslash Delta\; \backslash theta$ is the peak phase deviation. Compare to the modulation index for frequency modulation.

See also

* Angle modulation * Automatic frequency control * Modulation for a list of other modulation techniques * Modulation sphere * Polar modulation * Electro-optic modulator for Pockel's Effect phase modulation for applying sidebands to a monochromatic wave {{DEFAULTSORT:Phase Modulation Category:Radio modulation modes

Theory

PM changes the phase angle of the complex envelope in direct proportion to the message signal. If ''m(t)'' is the message signal to be transmitted and the carrier onto which the signal is modulated is :$c(t)\; =\; A\_c\backslash sin\backslash left(\backslash omega\_\backslash mathrmt\; +\; \backslash phi\_\backslash mathrm\backslash right).$, then the modulated signal is :$y(t)\; =\; A\_c\backslash sin\backslash left(\backslash omega\_\backslash mathrmt\; +\; m(t)\; +\; \backslash phi\_\backslash mathrm\backslash right).$ This shows how $m(t)$ modulates the phase - the greater m(t) is at a point in time, the greater the phase shift of the modulated signal at that point. It can also be viewed as a change of the frequency of the carrier signal, and phase modulation can thus be considered a special case of FM in which the carrier frequency modulation is given by the time derivative of the phase modulation. The modulation signal could here be :$m(t)\; =\; \backslash cos\backslash left(\backslash omega\_\backslash mathrm\; t\; +\; h\backslash omega\_\backslash mathrm(t)\backslash right)\backslash $ The mathematics of the spectral behavior reveals that there are two regions of particular interest: *For small amplitude signals, PM is similar to amplitude modulation (AM) and exhibits its unfortunate doubling of baseband bandwidth and poor efficiency. *For a single large sinusoidal signal, PM is similar to FM, and its bandwidth is approximately ::$2\backslash left(h\; +\; 1\backslash right)f\_\backslash mathrm$, :where $f\_\backslash mathrm\; =\; \backslash omega\_\backslash mathrm/2\backslash pi$ and $h$ is the modulation index defined below. This is also known as Carson's Rule for PM.

Modulation index

As with other modulation indices, this quantity indicates by how much the modulated variable varies around its unmodulated level. It relates to the variations in the phase of the carrier signal: :$h\backslash ,\; =\; \backslash Delta\; \backslash theta\backslash ,$, where $\backslash Delta\; \backslash theta$ is the peak phase deviation. Compare to the modulation index for frequency modulation.

See also

* Angle modulation * Automatic frequency control * Modulation for a list of other modulation techniques * Modulation sphere * Polar modulation * Electro-optic modulator for Pockel's Effect phase modulation for applying sidebands to a monochromatic wave {{DEFAULTSORT:Phase Modulation Category:Radio modulation modes