1. Introduction to Phase Modulation
Phase Modulation (PM) is an angle modulation technique where the phase of the carrier signal is varied in proportion to the amplitude of the modulating signal.
Where:
- Ac = Carrier amplitude
- fc = Carrier frequency
- kp = Phase sensitivity (rad/V)
- m(t) = Modulating signal
Figure 1 shows a sinusoidal message signal that is to be transmitted from an end to another, a carrier signal which is to be phase modulated. And the last image in the above figure represents the phase modulated signal.
Figure 1. Phase Modulation waveforms
From Figure 1, it is clear from the above figure that when the amplitude of the sinusoidal signal starts to increase and reaches the maximum value, then the phase lead of the carrier signal gets increased. Due to this a compression in the carrier signal is noticed. This resultantly increases the frequency of the signal. However, when the amplitude of the modulating signal starts falling and attains a minimum value, then the phase lag of the carrier wave occurs. Thereby resultantly causing stretching of the signal. Due to this, the frequency of the signal gets increased. So, in this way, we can say that with the change in phase of the signal during phase modulation, the frequency of the signal also shows some variation.
For a sinusoidal signal, the modulated signal is somewhat similar in case of both frequency and phase modulation. While in the case of the square wave signal, the case is not exactly the same as shown in Figure 2. For the case of the square wave, when the signal moves from positive to negative amplitude then negative phase reversal exists. While, when the message signal shows movement from negative to positive amplitude then positive phase reversal takes place. Therefore, it is not true that the frequency and phase modulated signal are similar for any type of waveform.
Figure 2. Square Wave FM and squarewave PM waveforms
PM vs. Frequency Modulation (FM)
PM: Phase changes with m(t)
FM: Frequency changes with m(t)
Note: PM and FM are related through the derivative/integral of m(t)
2. Mathematical Foundations
2.1 Phase Deviation
The peak phase deviation (Δφ):
For sinusoidal m(t) = Amcos(2πfmt):
2.2 Spectrum and Bandwidth
PM generates infinite sidebands described by Bessel functions:
Carson's Rule for bandwidth estimation:
3. Generation & Demodulation
3.1 PM Generation Methods
| Method | Description | Implementation |
|---|---|---|
| Direct | Vary phase directly using voltage-controlled phase shifter | Varactor diode, reactance modulator |
| Indirect | Integrate m(t) → FM modulator (Armstrong method) | Op-amp integrator + VCO |
3.2 PM Demodulation Techniques
- Phase-Locked Loop (PLL) - Most common method
- Differentiator + Envelope Detector - Convert PM to AM
- Product Detector - Multiplier + LPF
4. Key Properties
| Property | PM Characteristics |
|---|---|
| Noise Immunity | Better than AM, worse than FM |
| Bandwidth | Increases with modulation index (β) |
| Power Efficiency | Constant envelope → good for RF amplifiers |
| Implementation Complexity | Higher than AM, similar to FM |