Signal Analysis & Synthesis

Types of Signals

Signal Analysis

Fourier's Theorem

Analogue Modulation

DSB/SC

SSB/SC

FM

Phase Modulation

Analogue signal processing

Ideal Low-pass Filter

Real and Ideal Filters

Frequency conversion

Digital signal processing

Digital modulation

Pulse width

Pulse position

Pulse code

Communication Systems

FDMA

TDMA

Basic fiber

Interactive Exercise

Phase Modulation

As already mentioned, frequency modulation and phase modulation are very closely related and may be termed as Angle modulation. However, there exist some important differences between the two that warrant this discussion.


The process of phase modulation consists of varying the phase of the carrier linearly in proportion to the modulating signal such that maximum phase shift occurs during positive and negative peaks of the modulating signal. If ec is taken to represent the instantaneous value of the carrier, then

Where, is the initial phase of the wave.

Let the modulating signal be e = E sin t. If the carrier phase varies sinusoidal with the modulating signal, then the phase modulated wave is represented by

Assuming that initially the

Equation representing the phase modulated wave may be expanded in a way similar to FM. This expansion gives:

Where (m) is termed as the modulation index for phase modulation and equals .

The PM wave like FM waves have identical frequency spectrum. In PM, is given a fixed maximum value so that as the modulating frequency Fm varies, frequency deviation also varies and remain constant. This is different from FM

where is constant and can be given a large value. As signal to noise station at the

receiver output depends upon frequency deviation and not upon , FM is preferred to PM. However, this gives an indirect method of producing frequency modulated waves.

Phase Modulation Circuit

It should be remembered that FM and PM are closely related and may be termed as angle modulation. Because in both the cases, the changes in phase angle as well as frequency of the modulated carrier take place. Thus, consider a phase modulated wave given below:

Phase modulated wave

Where f(t) is the modulating signal.

The term under the bracket represents the instantaneous phase angle

Instantaneous angular velocity

Equation shows that in a PM wave, the frequency varies in proportion to the derivative of the modulating signal.

Now consider a frequency modulated wave given as,

Instantaneous angular velocity

The instantaneous phase change in the FM wave can be computed by integrating

the angular velocity

Where is a constant of integration.

The instantaneous phase angle in a frequency modulated wave varies directly as the integral of the modulating signal.

An important conclusion can be derived from the preceding discussion. If the modulating signal f(t) is integrated before using it to phase modulate a carrier, the result is an FM wave, similarly, if the modulating signal is differentiated before allowing it to frequency modulate a carrier, the result is a PM wave. An important characteristic of PM is that it does not require additional pre - emphasis and de - emphasis like FM. Hence it may be considered as an FM system with perfect pre - emphasis and de - emphasis.

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