PHASE LOCKED LOOPS

EE 458 LAB REPORT EXPERIMENT PHASE LOCKED LOOPS Purpose: The objectives of this laboratory are: To introduce students to Phase Locked Loops (PLL) and their operation To predict and measure the PLL characteristics To set up practical circuits using the PLL Equipment List PC with Matlab and Simulink The Phase Locked Loop Principle: The phase locked loop is a feedback system comprised of a phase comparator, a low pass filter and error amplifier in the forward signal path and a voltage-controlled oscillator (VC0) in the feedback path The block diagram of a basic PLL system is shown Perhaps the single most important point to realize when designing with the PLL is that it is a feedback system and, hence, is characterized mathematically by the same questions that apply to other, more conventional feedback systems The parameters in the equations are somewhat different, however since the feedback error signal in the phase locked system is related to phase rather than to current or voltage, as is usually the case in conventional feedback systems LOOP OPERATIONS: Figure A (a) PLL operation From a qualitative point of view, the basic principle of PLL operation can be briefly explained With no signal input applied to the system, the error voltage Ve is equal to The VCO operates at a set frequency wo, which is known as the free-running frequency If an input signal is applied to the system, the phase comparator compares the phase and frequency of the input signal with the VCO frequency and generates an error voltage Ve(t) that is related to the phase and the frequency difference between the two signals This error voltage is then filtered, amplified and applied to the control terminal of the VCO In this manner, the control voltage vd(t) forces the VCO frequency to vary in a direction that reduces the frequency difference between fo and the input signal If the input frequency wi is sufficiently close to wo, the feedback nature of the PLL causes the VCO to synchronize or lock with the incoming signal Once in lock, the VCO frequency is identical to the input signal except that for a finite phase difference Figure A (b) Input power spectrum This net phase difference is Θ is necessary to generate the corrective error voltage Vd to shift the VCO frequency from its free-running value to the input signal frequency wi and thus, keep the PLL in lock This self-correcting ability of the system also allows the PLL to track the frequency Figure A (c) Block parameters of input power spectrum The range of frequencies over which the PLL can maintain lock with an input signal is defined as the “lock range” of the system The band of frequencies over which the PLL can acquire lock with an incoming signal is called “Capture range” of the system and is never greater than the “lock range” Another means for describing the operation of the PLL is to observe that the phase detector is in actuality a multiplier circuit that mixes the input signal with the VCO signal This mix produces sum and difference frequencies wi +- w0 When the loop is in lock, the VCO duplicates the input frequency so that the difference frequency wi – wo is zero, hence the output of the phase comparator contains a dc component The low pass filter removes the sum frequency component wi + wo but passes the dc component, which is then amplified and fed back to the VCO Notice that when the loop is in lock, the difference frequency component is always dc, so the lock range is independent of the band edge of the low pass filter Figure A (d) Block parameters of Analog filter design LOCK AND CAPTURE: Figure A (e) Input scope Consider now the case where the loop is not yet in lock The phase comparator again mixes the input and VCO signals to produce sum and difference frequency components If the difference frequency is above the cut off frequency of the low pass filter, no signal is transmitted around the loop and the VCO remains at its initial free-running frequency As the input frequency approaches that of the VCO, the frequency of the difference component decreases and approaches the band edge of the low pass filter Now some of the difference component is passed, which tends to drice the VCO towards the frequency of the input signal This, in turn decreases the frequency of the difference component and allows more information to be transmitted through the low pass filter to the VCO This is essentially a positive feedback mechanism, which causes the VCO to snap into lock with the input signal With this mechanism in mind, the term, “Capture range” can again be defined as the frequency range centered about the VCO initial free-running frequency over which the loop can acquire lock with the input signal The capture range is a measure of how close the input signal’s frequency must be to that of the VCO to acquire lock The “capture range” can assume any value within the lock range and depends primarily upon the band edge of the low pass filter together with the closed loop gain of the system It is this signalcapturing phenomenon which gives the loop its frequency selective properties Figure A (f) Block parameters of VCO Figure A (g) Block parameters of error rate calculator Figure A (h) Output power spectrum It is important to distinguish the “capture range” from the “lock range” which can, again be defined as the frequency range usually centered about the VCO initial free-running frequency over which the loop can track the input signal once lock has been achieved When the loop is in lock, the difference frequency component on the output of the phase comparator (error voltage) is dc and will always be passes by the low pass filter Thus, the lock range is limited by the range of the error voltage that can be generated (Vd) and the corresponding VCO frequency deviation delta wo produced The lock range is essentially a dc parameter and is not affected by the band edge of the low pass filter Frequency Tracking: Figure shows the typical frequency-to-voltage transfer characteristics of the PLL The input is assumed to be a sine wave whose frequency is swept slowly over a broad frequency range The vertical scale is the corresponding loop error voltage The top figure shows the input frequency being gradually increased The loop doesn’t respond to the signal until it a frequency w1, corresponding to the lower edge of the capture range Then, the loop suddenly licks on the input and causes a negative jump of the loop error voltage Next Vd varies with frequency with a slope equal to the reciprocal of VCO gain (1/ Ko) and goes through zero as wi = wo The loop tracks the input until the input frequency reaches w2, corresponding to the upper edge of the lock renge The PLL then loses lock and the erro voltage drops to zero If the input frequency is swept slowly back now, the cycle repeats itself, but it is inverted, as shown in the lower fig The loop recaptures the signal at w3 and tracks it down to w4 The total capture and lock ranges of the system are: 2wc = w3 – w1 and 2wL = w2 – w4 Note that the PLL system has an inherent selectivity about the center frequency set by the VCO free-running frequency wo It will respond only to the input signal frequencies that are separated from w0 by less than wL or Wc, depending on whether the loop starts with or without an initial lock condition The linearity of the frequency-to-voltage conversion characteristics for the PLL is determined solely by the VCO conversion gain Therefore, in most PLL application, the VCIO is required to have highly linear voltage-to-frequency characteristics Measuring Constants We started our experiment on PLLs by first measuring the different parameters of each functional block Multiplier Constant, Km With a 1V p-p sinusoidal voltage at both inputs of the multiplier, the output was observed and the multiplier constant was calculated to be 0.206 Phase Detector Constant, Kd The phase detector consists of an analog multiplier and a limiter to remove the amplitude variations in the input signal Kd = peak output voltage of the limiter * peak voltage of the VCO * multiplier constant Kd = (1.86 x √2) x (2.199 x √2) x 0.206 ∴Kd = 1.72 volts VCO Conversion Constant, Ko An external voltage may control the output frequency of the VCO The change in the output frequency per change in the dc input voltage was measured Ko = Δf / Δv Ko = / 0.5 = kHz/sec/volt ∴Ko = 4π103 = 12566 rad/sec/volt Total Loop Gain, KT KT = Kd x Ko = 1.72 x 12566 = 21613.52 Low Pass Filter Two first-order low pass filters are used The cutoff frequencies for one of the low pass filters is 100Hz and the other is 1kHz This was verified by using the white noise as the signal source and then checking the filter output spectrum on the spectrum analyzer The power spectral density for the white noise is uniform at input – i.e., power of equal amplitude exists approximately at all frequencies In the output spectrum, the roll off occurred at approximately 100 Hz and 1kHz respectively The spectrum analyzer was configured to act as the source of random white noise To obtain the maximum noise output, the attenuation level was set to dB This was fed to the low pass filters and the output was observed on the spectrum analyzer The same procedure was repeated for the 4th order low pass filter In this case, the filter knob was adjusted so that the dB roll off occurred approximately at kHz Phase Lock Loop Operation The circuit is connected as shown in the schematic The open loop system is closed and using a jumper around it by-passes the filter The capture and the lock ranges for the PLL are calculated By varying the Philips frequency, and using a frequency counter along with the DC voltmeter, the capture and the lock ranges are measured The signals within the PLL are observed on the oscilloscope The above steps are repeated using the 1kHz cut off low pass filter and then the 100 Hz cut off low pass filter Calculations: The values of Lock and Capture Range obtained by calculations were: Lock Range: 2ωL = 2KT 2fL = KT / π = 6880 Hz Capture Range: 2fC = 2√ fL * f3 Using a 100 Hz cutoff 1st order low pass filter, f3 = 100Hz ∴ 2fC = √ 6880 * 100 = 1660 Hz Using a 1000 Hz cutoff 1st order low pass filter, f3 = 1000 Hz ∴ 2fC = √ 6880 * 1000 = 5245 Hz Observations: The values of the Lock Range and Capture Range obtained by the experiment are: Lock Range: 2fL = 8.4 kHz – 1.6 kHz = 6.8 kHz Capture Range: Using a 100 Hz cutoff 1st order low pass filter, 2fC = 5.66 kHz – 4.37 kHz = 1.29 kHz Using a 1000 Hz cutoff 1st order low pass filter, 2fC = 7.7 kHz – 2.7 kHz = 5.0 kHz PLL With “Locked” Indicator The circuit is connected as shown in the schematic This is a method of indicating if a PLL is in its “locked” condition Since the output of the phase detector tends toward zero, multiplication of the input signal by a 90° shifted VCO signal (QUAD) tends to be maximum The DC component of this maximum signal was used to light a L.E.D, indicating that it is in the locked state As connected, it was difficult to light the LED while the loop is in the locked state Hence, we swapped the TTL and the QUAD outputs of the VCO Now we were able to get the LED to light up when the PLL was in the locked state Figure B (a) PLL with lock operation Figure B (b) Block parameters to implement a diiode Figure B (c) Block parameters of VCO Quad Figure B (d) Slider gain as part of the limiter Figure B (e) Input power spectrum Figure B (f) Input scope Figure B (g) Output power spectrum Figure B (h) Scope reading AM Detection without Transmitter Reference PLL can have a rather narrow bandwidth We could use this feature to “pick off” a carrier signal from between the two side bands in the case of AM signals The PLL is now locked on to the carrier’s frequency If the limiter were removed, the PLL would still be locked to the carrier’s phase Thus, we have a method for coherent demodulation for AM and DSB with a small pilot carrier We rigged up a circuit for the AM / DSBSC transmitter The carrier frequency was set for kHz and modulated at kHz In the open loop condition, the VCO (used for the detection) was set to approximately kHz, which is close to the carrier frequency The 2nd LPF cut off frequency was set to approximately kHz The loop was closed and the detector output was observed The detector was able to receive the AM wave quite well at both 50% modulation and 100% modulation figure C (a) Modulated input figure C (b)Ouput before feeding it to the LPF figure C (c)Slider gain part of limiter figure C (d) Am detect spectrum analyzer figure C (d) Recovered Signal Appendix I Prelab I A 1st order LPF is used in a PLL and has a magnitude response of : | F(f) | = sqrt( / + (f/f3)2) To show that the capture range is 2fc = sqrt(fLf3) In KD Fs Ko VCO Lock Range: 2ωL = KT T(s) = KT F(s) / S Total loop gain = Kd A Ko 2fL = KT / π Capture Range τ = RC where τ = / 2πf3 2ωc = sqrt(KT / τ ) (2π fc ) = 2sqrt(2πfL / (1/ 2πf3)) = sqrt((2π)2 fL f3) 2fc = 2sqrt(fL f3) A II Lock Range: 2fL = KT / π Capture Range: 2fc = 2sqrt(fL f3) Ka = 2V Ko = kHz /v A = f3 = 100Hz KT = Kd A Ko = (2V) (2 x 103 Hz / V) (1) = 4kHz Lock: = 2fL = KT / π = 4kHz / π = 1.273 k = 637 Hz Capture: = 2fc = 2sqrt(fL f3) = 2sqrt(637x100) = 504.6 Hz - fc = 252 Hz III VCO(t) = sin(wot + ∅ ) VIN(t) = 0.2 cos(wot) ∅e(t) = 0.2 sin(wot + ∅) cos(wot) ; Km = Kd = 0.2 at max KT = Kd A K0 = (0.2)(2x103 Hz / V) (1) = 400 Hz Lock: = 2fL = KT / π = 400 / π fL = 6306 Hz Capture: 2fc = 2sqrt(fLf3) = 2sqrt(6306x100) fc = 80 Hz Limter O/p: 4.72 Vpp VCO O/p : 3076 Vpp Multiplier’s Constant: 0.408 Kd = (4.72 / 2) x (3.76 / 2) x 0.408 = 1.81 V Avg VCO Conversion: Δ fo / ΔVa = -2.08 kHz / V ... to Phase Locked Loops (PLL) and their operation To predict and measure the PLL characteristics To set up practical circuits using the PLL Equipment List PC with Matlab and Simulink The Phase Locked. .. List PC with Matlab and Simulink The Phase Locked Loop Principle: The phase locked loop is a feedback system comprised of a phase comparator, a low pass filter and error amplifier in the forward... equations are somewhat different, however since the feedback error signal in the phase locked system is related to phase rather than to current or voltage, as is usually the case in conventional