The general block diagram of a Phase Locked Loop (P.L.L.) includes several subsystems:
Phase Detector (PD): Outputs a voltage proportional to the phase difference between the input and the V.C.O.
Equation: Vd = KD (\theta{in} - \theta{out})
Loop Filter (LF): Smooths the output of the PD to control the V.C.O.
Function: Filters the error signal to produce a control voltage.
Voltage Controlled Oscillator (V.C.O.): Generates a signal whose frequency is controlled by an input voltage.
Output: V{out} = A \cos(\omega{o} t + \phi)
Frequency Divider (÷ N): Reduces the frequency of the oscillator output for synchronization purposes.
The output voltage of the phase detector is defined by:
Output: Vd = KD \cdot e
Where: K_D = [V/rad]
Input signals can be represented as:
V1(t) = A \sin(\omega1 t + \phi_1)
V2(t) = B \cos(\omega0 t + \phi_0)
The Loop Filter stabilizes the response of the P.L.L.
Passive Loop Filter:
Transfer Function: F_1(S) = \frac{1}{\tau + 1}
Active Loop Filter:
More complex with multiple poles and zeros designed to optimize bandwidth and stability.
The frequency response of a V.C.O. is defined by:
f{VCO} = \text{Control Voltage} \cdot K0
Deviation from center frequency: \Delta \omega = K0 \cdot Ve \cdot \frac{dV_e}{dt}
The relationship between input voltage and output can be modeled in the Laplace domain as:
V1(s) = KO rac{KD}{N} F(s) imes Ve(s)
Closed-loop transfer function can be represented as:
H(s) = \frac{K{O} K{D} / N imes F(s)}{s + KO KD / N imes F(s)}
Where:
K' = KO KD / N
H(s) is fundamental to understanding stability and response in feedback systems.
Divides the output of the V.C.O. by integer values of N, allowing access to a range of clock frequencies:
\theta(t) = A \cos(\omega_0 t + \phi)
The P.L.L. operates as a narrowband filter, improving selectivity and noise rejection:
Loop noise bandwidth, B_L = \sqrt{\int |H(j\omega)|^2 d\omega}
Conditions for locking depend on input signal frequencies and loop bandwidth:
Locking occurs when input phase/frequency is within loop filter bandwidth.
Pull-in frequency difference: \Delta \omega{max} = \frac{K'}{25 \omegan}
Time to achieve synchronization is a function of various parameters:
Average acquisition time, TA = \frac{1.3}{BL}
Factors affecting this include the initial frequency offset.
A practical example includes designing a synchronizer that can acquire signals within a defined number of symbol periods.
Loop parameters are critical, e.g., damping factor, mean acquisition time, and loop division factor must be calculated correctly.
Loop Bandwidth adjustments are crucial for both initial acquisition and synchronization stability:
Bandwidth should be broader during acquisition and tapered down for stable operation.
Selecting external components like resistors and capacitors effectively tunes the loop filter for desired performance:
Utilize manufacturer curves and specifications for components to determine suitable values.
Commonly involves a combination of timing circuits and logic gates for digital implementations.
Key texts for further study include:
K. Feher - Digital Communications: Microwave Applications
WR Bennett, Jr. - Data Transmission
WC Lindsey and M. K. Simon - Telecommunication Systems Engineering
FM Gardner - Phaselock Techniques
A. Viterbi - Principles of Coherent Communication