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PHASE LOCKED LOOP APPLICATIONSWhen operated from dual symmetrical supplies, the squarewave on pin 4 will swing between a low level of slightly(0.2V) below ground to a high level of one diode voltagedrop (O.7V) below positive supply. The triangle waveform on pin 9 is approximately centered between positiveand negative supply and has an amplitude of 2V withsupply voltages of ±5V. The amplitude of the trianglewaveform is directly proportional to the supply voltages.The phase detector is again of the doubly-balancedmodulator type. Transistors 020 and 024 form the signalinput stage, and must be biased externally. If dualsymmetrical supplies are used, it is simplest to bias 020and 024 through external resistors to ground. Theswitching stage 018, 019, 022 and 023 is driven from theSchmitt trigger via pin 5 and Dll. Diodes D12 and D13limit the phase detector output, and differential amplifier026 and 027 provides increased loop gain.The loop low pass filter is formed with an externalcapacitor (connected to pin 7) and the collector resistanceR24 (typically 3.6r2). The voltage on pin 7 becomes theerror voltage which is then connected back to the controlvoltage terminal of the VCO (base of 01). Pin 6 isconnected to a tap on the bias resistor string and providesa reference voltage which is nominally equal to the outputvoltage on pin 7. This allows differential stages to be bothbiased and driven by connecting them to pins 6 and 7.The free-running center frequency of the 565 is adjustedby means of R 1 and Cl and is given approximately by1.2f ~-­o4R1ClWhen the phase comparator is in the limiting mode(Vin ~ 200mV p-p), the lock range can be calculated fromthe expression:2wL = 2KoKdAOdThe lock range for the 565 then becomes:to each side of the center frequency, or a total range of:16f o2fL :::: -- HzVccThe capture range, over which the loop can acquire lockwith the input signal is given approximately by:where W L is the one-sided lock rangeand T is the time constant of the loop filterT = RC2with R = 3.6kr2.This can be written as:to each side of the center frequency or a total capturerange of:fc '" ~ J1T321TfOTV ccThis approximation works well for narrow capture ranges(fc = 1/3fL) but becomes too large as the limiting case isapproached (fc = f L ).where Ko is the VCO conversion gain, Kd is the phasedetector gain factor, A is the amplifier gain and Bd is themaximum phase error over which the loop can remain inlock.DETAILED DESCRIPTION OF 56650f oFor the 565: Ko =Vccradians/sec/volt(where fo is the free-running frequency of the VCO andV cc is the total supply voltage applied to the circuit.)Kd1.41TA 1.4°d1T2volts/radianradiansThe 566 is the voltage controlled oscillator portion of the565. The basic die is the same as that of the 565; modifiedmetalization is used to bring out only the VCO. The 566circuit diagram is shown in Figure 8-31. Transistor 018has been a buffered triangle waveform output. (The trianglewaveform is available at capacitor Cl also, but any currentdrawn from pin 7 will alter the duty cycle and frequency.)The square wave output is available from 019 by pin 4. Thecircuit will operate at frequencies up to 1 MHz and may beprogrammed by the voltage applied on the control terminal(pin 5), current injected into pin 6 or the value of theexternal resistor and capacitor (R 1 and C 1).37

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