Order this document by MC145149/D SEMICONDUCTOR TECHNICAL DATA Interfaces with Dual–Modulus Prescalers The MC145149 contains two PLL Frequency Synthesizers which share a common serial data port and common reference oscillator. The device contains two 14–stage R counters, two 10–stage N counters, and two 7–stage A counters. All six counters are fully programmable through a serial port. The divide ratios are latched into the appropriate counter latch according to the last data bits (control bits) entered. When combined with external low–pass filters and voltage controlled oscillators (VCOs), the MC145149 can provide all the remaining functions for two PLL frequency synthesizers operating up to the device’s frequency limit. For higher VCO frequency operation, a down mixer or dual–modulus prescaler can be used between the VCO and the synthesizer IC. • • • • • • • • • • Low Power Consumption Through Use of CMOS Technology Wide Operating Voltage Range: 3 to 9 V Operating Temperature Range: – 40 to + 85°C ÷ R Range = 3 to 16,383 ÷ N Range = 3 to 1023 ÷ A Range = 0 to 127 Two “Linearized” Three–State Digital Phase Detectors with No Dead Zone Two Lock Detect Signals (LD1 and LD2) Two Open–Drain Port Expander Outputs (SW1 and SW2) Compatible with the Serial Peripheral Interface (SPI) on CMOS MCUs Motorola, Inc. 1995 MOTOROLA P SUFFIX PLASTIC DIP CASE 738 20 1 DW SUFFIX SOG PACKAGE CASE 751D 20 1 ORDERING INFORMATION MC145149P Plastic DIP MC145149DW SOG Package PIN ASSIGNMENT LD1 1 20 VSS1 MC1 2 19 PDout1 ENB 3 18 VDD1 fin1 4 17 SW1 DATA 5 16 OSCout CLK 6 15 OSCin fin2 7 14 SW2 S/Rout 8 13 VDD2 MC2 9 12 PDout2 LD2 10 11 VSS2 MC145149 1 BLOCK DIAGRAM 17 1–BIT LATCH PIN 18 = VDD1 PIN 20 = VSS1 14–BIT SHIFT REGISTER ENB 3 SW1 14 LOCK DETECT REFERENCE COUNTER LATCH 1 LD1 14 fR 14–BIT ÷ R COUNTER PHASE DETECTOR CONTROL LOGIC fin1 4 7–BIT ÷ A COUNTER 10–BIT ÷ N COUNTER 7 1–BIT CONTROL S/R OSCin 15 OSCout 16 fV 10 ÷ N COUNTER LATCH 7 ÷ A COUNTER LATCH 2 MODULUS CONTROL 1 (MC1) 10 7–BIT S/R 19 PDout1 10–BIT S/R PLL1 PLL2 14 1–BIT LATCH SW2 PIN 13 = VDD2 PIN 11 = VSS2 14–BIT SHIFT REGISTER 14 LOCK DETECT REFERENCE COUNTER LATCH 10 LD2 14 fR 14–BIT ÷ R COUNTER PDout2 CONTROL LOGIC PHASE DETECTOR fin2 7 7–BIT ÷ A COUNTER DATA CLK 5 6 MC145149 2 7 ÷ A COUNTER LATCH 2–BIT CONTROL S/R 1–BIT CONTROL S/R 7 7–BIT S/R 12 10–BIT ÷ N COUNTER 10 ÷ N COUNTER LATCH fV 9 MODULUS CONTROL 2 (MC2) 10 10–BIT S/R 8 S/Rout MOTOROLA MAXIMUM RATINGS* (Voltages Referenced to VSS) Symbol VDD Rating DC Supply Voltage Value Unit – 0.5 to + 10 V Vin, Vout Input or Output Voltage (DC or Transient) except SW1, SW2 – 0.5 to VDD + 0.5 V Vout Output Voltage (DC or Transient) — SW1, SW2 – 0.5 to 15 V Iin, Iout Input or Output Current (DC or Transient), per Pin ± 10 mA IDD, ISS Supply Current, VDD or VSS Pins ± 30 mA PD Power Dissipation, per Package† 500 mW Tstg Storage Temperature – 65 to + 150 °C 260 °C TL Lead Temperature (8–Second Soldering) This device contains circuitry to protect against damage due to high static voltages or electric fields, however, it is advised that normal precautions be taken to avoid applications of any voltage higher than maximum rated voltages to this high–impedance circuit. For proper operation, it is recommended that Vin and Vout be constrained to the range VSS ≤ (Vin or Vout) ≤ VDD except SW1 and SW2 which may range up to 15 V. Unused inputs must always be tied to an appropriate logic voltage level (e.g., either VSS or VDD). Unused outputs should be left floating. * Maximum Ratings are those values beyond which damage to the device may occur. †Power Dissipation Temperature Derating: Plastic DIP: – 12 mW/°C from 65 to 85°C SOG Package: – 7 mW/°C from 65 to 85°C ELECTRICAL CHARACTERISTICS (Voltages Referenced to VSS) S b l Symbol Ch i i Characteristic VDD Power Supply Voltage Range VOL Output Voltage Vin = 0 V or VDD Iout = 0 µA VOH VIL Input Voltage Vout = 0.5 V or VDD – 0.5 V (All Outputs Except OSCout) VIH IOH Output Current — MC1, MC2 Vout = 2.7 V Vout = 4.6 V Vout = 8.5 V IOL IOL IOH VDD V Vout = 0.3 V Vout = 0.4 V Vout = 0.5 V Output Current — SW1, SW2 Vout = 0.3 V Vout = 0.4 V Vout = 0.5 V Output Current — Other Outputs Vout = 2.7 V Vout = 4.6 V Vout = 8.5 V IOL Vout = 0.3 V Vout = 0.4 V Vout = 0.5 V – 40°C Min 25°C Max Min 85°C Max Min Max U i Unit — 3 9 3 9 3 9 V 0 Level 3 5 9 — — — 0.05 0.05 0.05 — — — 0.05 0.05 0.05 — — — 0.05 0.05 0.05 V 1 Level 3 5 9 2.95 4.95 8.95 — — — 2.95 4.95 8.95 — — — 2.95 4.95 8.95 — — — 0 Level 3 5 9 — — — 0.9 1.5 2.7 — — — 0.9 1.5 2.7 — — — 0.9 1.5 2.7 1 Level 3 5 9 2.1 3.5 6.3 — — — 2.1 3.5 6.3 — — — 2.1 3.5 6.3 — — — Source 3 5 9 – 0.60 – 0.90 – 1.50 — — — – 0.50 – 0.75 – 1.25 — — — – 0.30 – 0.50 – 0.80 — — — Sink 3 5 9 1.30 1.90 3.80 — — — 1.10 1.70 3.30 — — — 0.66 1.08 2.10 — — — Sink 3 5 9 0.80 1.50 3.50 — — — 0.48 0.90 2.10 — — — 0.24 0.45 1.50 — — — Source 3 5 9 – 0.44 – 0.64 – 1.30 — — — – 0.35 – 0.51 – 1.00 — — — – 0.22 – 0.36 – 0.70 — — — Sink 3 5 9 0.44 0.64 1.30 — — — 0.35 0.51 1.00 — — — 0.22 0.36 0.70 — — — V mA mA mA Iin Input Current — DATA, CLK, ENB 9 — ± 0.3 — ± 0.1 — ± 1.0 µA Iin Input Current — fin, OSCin 9 — ± 50 — ± 25 — ± 22 µA (continued) MOTOROLA MC145149 3 ELECTRICAL CHARACTERISTICS (continued) – 40°C 25°C 85°C VDD V Min Max Min Max Min Max U i Unit Input Capacitance — — 10 — 10 — 10 pF Cout Three–State Output Capacitance — PDout — — 10 — 10 — 10 pF IDD Quiescent Current Vin = 0 V or VDD Iout = 0 µA 3 5 9 — — — 800 1200 1600 — — — 800 1200 1600 — 1600 2400 3200 µA IOZ Three–State Leakage Current — PDout Vout = 0 V or 9 V 9 — ± 0.3 — ± 0.1 — ± 3.0 µA IOZ Off–State Leakage Current — SW1, SW2 Vout = 9 V 9 — 0.3 — 0.1 — 3.0 µA S b l Symbol Cin Ch Characteristic i i SWITCHING CHARACTERISTICS (TA = 25°C, CL = 50 pF) Symbol Characteristic Figure No. VDD V Min Max Unit tTLH Output Rise Time, MC1 and MC2 1, 6 3 5 9 — — — 115 60 40 ns tTHL Output Fall Time, MC1 and MC2 1, 6 3 5 9 — — — 60 34 30 ns tTLH, tTHL Output Rise and Fall Time, LD and S/Rout 1, 6 3 5 9 — — — 140 80 60 ns tPLH, tPHL Propagation Delay Time, fin to MC1 or MC2 2, 6 3 5 9 — — — 125 80 50 ns tsu Setup Time, DATA to CLK 3 3 5 9 30 20 18 — — — ns tsu Setup Time, CLK to ENB 3 3 5 9 70 32 25 — — — ns th Hold Time, CLK to DATA 3 3 5 9 12 12 15 — — — ns trec Recovery Time, ENB to CLK 3 3 5 9 5 10 20 — — — ns tr, tf Input Rise and Fall Times, Any Input 4 3 5 9 — — — 5 2 0.5 µs Input Pulse Width, ENB and CLK 5 3 5 9 40 35 25 — — — ns tw MC145149 4 MOTOROLA FREQUENCY CHARACTERISTICS (Voltages Referenced to VSS, CL = 50 pF, Input tr = tf = 10 ns unless otherwise indicated) S b l Symbol fi P Parameter 25°C 85°C Min Max Min Max Min Max U i Unit R ≥ 8, A ≥ 0, N ≥ 8 Vin = 500 mV p–p ac coupled sine wave 3 5 9 — — — 6 15 15 — — — 6 15 15 — — — 6 15 15 MHz R ≥ 8, A ≥ 0, N ≥ 8 Vin = VDD to VSS dc coupled square wave 3 5 9 — — — 6 15 15 — — — 6 15 15 — — — 6 15 15 MHz T Test C Conditions di i Input Frequency (fin, OSCin) – 40°C VDD V SWITCHING WAVEFORMS VDD fin tTLH ANY OUTPUT 50% tPLH tTHL 90% 10% MC VSS tPHL 50% Figure 1. Figure 2. VDD DATA 50% VSS th tsu VDD CLK 50% LAST CLK FIRST CLK tsu trec VDD ENB tf tr VSS ANY INPUT VDD 90% 10% VSS 50% VSS Figure 4. PREVIOUS DATA LATCHED Figure 3. OUTPUT tw ENB, CLK VDD DEVICE UNDER TEST CL* 50% VSS * Includes all probe and fixture capacitance. Figure 5. MOTOROLA Figure 6. MC145149 5 PIN DESCRIPTIONS INPUT PINS OSCin, OSCout Reference Oscillator Input/Output (Pins 15, 16) These pins form a reference oscillator when connected to terminals of an external parallel–resonant crystal. Frequency–setting capacitors of appropriate value must be connected from OSCin and OSCout to ground. OSCin may also serve as input for an externally–generated reference signal. The signal is typically ac coupled to OSCin, but for signals with CMOS logic levels, dc coupling may be used. When used with an external reference, OSCout should be left open. fin1, fin2 Frequency Inputs (Pins 4, 7) Input frequency from an external VCO output. Each rising– edge signal on fin1 decrements the N counter, and when appropriate, the A counter of PLL 1. Similarly, fin2 decrements the counters of PLL 2. These inputs have inverters biased on the linear region which allows ac coupling for signals as low as 500 mV p–p. With square wave signals which swing from VSS to VDD, dc coupling may be used. DATA, CLK Data, Clock Inputs (Pins 5, 6) Shift register data and clock inputs. Each low–to–high transition on the clock pin shifts one bit of data into the on– chip shift registers. Refer to Figure 7 for the following discussion. The last bit entered is a steering bit that determines which set of latches are activated. A logic high selects the latches for PLL 1. A logic low selects PLL 2. The second–to–last bit controls the appropriate port expander output, SW1 or SW2. A logic low forces the output low. A logic high forces the output to the high–impedance state. The third–to–last bit determines which storage latch is activated. A logic low selects the ÷ A and ÷ N counter latches. A logic high selects the reference counter latch. When writing to either set of ÷ A and ÷ N counter latches, 20 clock cycles are typically used. However, if a byte– oriented MCU is utilized, 24 clock cycles may be used with the first 4 bits being “Don’t Care.” When writing to either reference counter latch, 17 clock cycles are typically used. However, if a byte–oriented MCU is utilized, 24 clock cycles may be used with the first 7 bits being “Don’t Care”. ENB Latch Enable Input (Pin 3) A positive pulse on this input transfers data from the shift registers to the selected latches, as determined by the control and steering data bits. A logic low level on this pin allows the user to shift data into the shift registers without affecting the data in the latches or counters. Enable is normally held low and is pulsed high to transfer data into the latches. MC145149 6 OUTPUT PINS PDout1, PDout2 Single–Ended Phase Detector Outputs (Pins 19, 12) Each single–ended (three–state) phase detector output produces a loop error signal that is used with a loop filter to control a VCO (see Figure 8). Frequency fV > fR or fV Leading: Negative Pulses Frequency fV < fR or fV Lagging: Positive Pulses Frequency fV = fR and Phase Coincidence: High–Impedance State S/Rout Shift Register Output (Pin 8) This output can be connected to an external shift register to provide band switching or control information. S/Rout may also be used to check the counter programming bit stream. MC1, MC2 Modulus Control Outputs (Pins 2, 9) Each output generates a signal by the on–chip control logic circuitry for controlling an external dual–modulus prescaler. The modulus control level is low at the beginning of a count cycle and remains low until the ÷ A counter has counted down from its programmed value. At this time, modulus control goes high and remains high until the ÷ N counter has counted the rest of the way down from its programmed value (N–A additional counts since both ÷ N and ÷ A are counting down during the first portion of the cycle). Modulus control is then set back low, the counters are preset to their respective programmed values, and the above sequence is repeated. This provides for a total programmable divide value (NT) = N • P + A where P and P + 1 represent the dual–modulus prescaler divide values respectively for high and low modulus control levels, N the number programmed into the ÷ N counter, and A the number programmed into the ÷ A counter. Note that when a prescaler is needed, the dual–modulus version offers a distinct advantage. The dual–modulus prescaler allows a higher reference frequency at the phase detector input, increasing system performance capability, and simplifying the loop filter design. LD1, LD2 Lock Detect Signals (Pins 1, 10) Each output is essentially at a high logic level when the corresponding loop is locked (fR and fV of the same phase and frequency). Each output pulses low when the corresponding loop is out of lock (see Figure 8). SW1, SW2 Latched Open–Drain Switch Outputs (Pins 17, 14) The state of each output is controlled by the “SW STATE” bit shown in Figure 7. If the bit is a logic high, the corresponding SW output assumes the high–impedance state. If the bit is low, the SW output goes low. To control output SW1, steering bit PLL 1/PLL 2 shown in Figure 7 must be high. To control SW2, bit PLL 1/PLL 2 must be low. These outputs have an output voltage range of VSS to 15 V. MOTOROLA For optimum performance, VDD1 should be bypassed to VSS1 and VDD2 bypassed to VSS2. That is, two separate bypass capacitors should be utilized. POWER SUPPLY PINS VDD1, VDD2 Positive Power Supply (Pins 18, 13) VSS1, VSS2 Negative Power Supply (Pins 20, 11) The most positive power supply potentials. Both of these pins are connected to the substrate of the chip. Therefore, both must be tied to the same voltage potential. This potential may range from 3 to 9 V with respect to the VSS pins. The most negative power supply potentials. Both of these pins should be tied to ground. MSB LSB SW STATE HIGH OR “1” PLL 1/PLL 2 ÷R LAST BIT INTO SHIFT REGISTER MSB LSB ÷N MSB LSB LOW OR “0” SW STATE PLL 1/PLL 2 ÷A LAST BIT INTO SHIFT REGISTER Figure 7. Bit Stream Formats fR REFERENCE (OSC ÷ R) fV FEEDBACK (fin ÷ N) PDout LD NOTE: The PD output state is equal to either VDD or VSS when active. When not active, the output is high impedance and the voltage at that pin is determined by the low–pass filter capacitor. Figure 8. Phase Detector/Lock Detector Output Waveforms MOTOROLA MC145149 7 A) PDout VCO ωn = R1 C B) PDout VCO ζ = Nωn 2KφKVCO F(s) = 1 R1sC + 1 ωn = R1 KφKVCO NR1C KφKVCO NC(R1 + R2) R2 ζ = 0.5 ωn C F(s) = ǒ N R2C + KφKVCO Ǔ R2sC + 1 (R1 + R2)sC + 1 DEFINITIONS: N = Total Division Ratio in Feedback Loop Kφ (Phase Detector Gain) = VDD/4π for PDout 2π∆fVCO KVCO (VCO Gain) = ∆VVCO 2πfr for a typical design ωn (Natural Frequency) ≈ (at phase detector input). 10 Damping Factor: ζ [1 RECOMMENDED READING: Gardner, Floyd M., Phaselock Techniques (second edition). New York, Wiley–Interscience, 1979. Manassewitsch, Vadim, Frequency Synthesizers: Theory and Design (second edition). New York, Wiley–Interscience, 1980. Blanchard, Alain, Phase–Locked Loops: Application to Coherent Receiver Design. New York, Wiley–Interscience, 1976. Egan, William F., Frequency Synthesis by Phase Lock. New York, Wiley–Interscience, 1981. Rohde, Ulrich L., Digital PLL Frequency Synthesizers Theory and Design. Englewood Cliffs, NJ, Prentice–Hall, 1983. Berlin, Howard M., Design of Phase–Locked Loop Circuits, with Experiments. Indianapolis, Howard W. Sams and Co., 1978. Kinley, Harold, The PLL Synthesizer Cookbook. Blue Ridge Summit, PA, Tab Books, 1980. AN535, Phase–Locked Loop Design Fundamentals, Motorola Semiconductor Products, Inc., 1970. AR254, Phase–Locked Loop Design Articles, Motorola Semiconductor Products, Inc., Reprinted with permission from Electronic Design, 1987. Figure 9. Phase–Locked Loop Low–Pass Filter Design DESIGN CONSIDERATIONS CRYSTAL OSCILLATOR CONSIDERATIONS The following options may be considered to provide a reference frequency to Motorola’s CMOS frequency synthesizers. Use of a Hybrid Crystal Oscillator Commercially available temperature–compensate crystal oscillators (TCXOs) or crystal–controlled data clock oscillators provide very stable reference frequencies. An oscillator capable of sinking and sourcing 50 µA at CMOS logic levels may be direct or dc coupled to OSCin. In general, the highest frequency capability is obtained utilizing a direct–coupled square wave having a rail–to–rail (VDD to VSS) voltage swing. If the oscillator does not have CMOS logic levels on the outputs, capacitive or ac coupling to OSCin may be used. OSCout, an unbuffered output, should be left floating. MC145149 8 For additional information about TCXOs and data clock oscillators, please consult the latest version of the eem Electronic Engineers Master Catalog, the Gold Book, or similar publications. Design an Off–Chip Reference The user may design an off–chip crystal oscillator using ICs specifically developed for crystal oscillator applications, such as the MC12061 MECL device. The reference signal from the MECL device is ac coupled to OSCin. For large amplitude signals (standard CMOS logic levels), dc coupling is used. OSCout, an unbuffered output, should be left floating. In general, the highest frequency capability is obtained with a direct–coupled square wave having rail–to–rail voltage swing. Use of the On–Chip Oscillator Circuitry The on–chip amplifier (a digital inverter) along with an appropriate crystal may be used to provide a reference source frequency. A fundamental mode crystal, parallel resonant at MOTOROLA the desired operating frequency, should be connected as shown in Figure 10. For VDD = 5.0 V, the crystal should be specified for a loading capacitance, CL, which does not exceed 32 pF for frequencies to approximately 8 MHz, 20 pF for frequencies in the area of 8 to 15 MHz, and 10 pF for higher frequencies. These are guidelines that provide a reasonable compromise between IC capacitance, drive capability, swamping variations in stray and IC input/output capacitance, and realistic C L values. The shunt load capacitance, C L , presented across the crystal can be estimated to be: CL = OSCin R1* C1 CinCout + Ca + CO + C1 • C2 C1 + C2 Cin + Cout where Cin = 5 pF (see Figure 11) Cout = 6 pF (see Figure 11) Ca = 1 pF (see Figure 11) CO= the crystal’s holder capacitance (see Figure 12) C1 and C2 = external capacitors (see Figure 10) The oscillator can be “trimmed” on–frequency by making a portion or all of C1 variable. The crystal and associated components must be located as close as possible to the OSCin and OSCout pins to minimize distortion, stray capacitance, stray inductance, and startup stabilization time. In some cases, stray capacitance should be added to the value for Cin and Cout. Power is dissipated in the effective series resistance of the crystal, Re, in Figure 12. The drive level specified by the crystal manufacturer is the maximum stress that a crystal can withstand without damaging or excessive shift in frequency. R1 in Figure 10 limits the drive level. The use of R1 may not be necessary in some cases (i.e., R1 = 0 Ω). To verify that the maximum dc supply voltage does not overdrive the crystal, monitor the output frequency as a function of voltage at OSCout. (Care should be taken to minimize loading.) The frequency should increase very slightly as the dc supply voltage is increased. An overdriven crystal will decrease in frequency or become unstable with an increase in supply voltage. The operating supply voltage must be reduced or R1 must be increased in value if the overdriven condition exists. The user should note that the oscillator start–up time is proportional to the value of R1. Through the process of supplying crystals for use with CMOS inverters, many crystal manufacturers have developed expertise in CMOS oscillator design with crystals. Discussions with such manufacturers can prove very helpful (see Table 1). FREQUENCY SYNTHESIZER Rf OSCout C2 * May be deleted in certain cases. See text. Figure 10. Pierce Crystal Oscillator Circuit Ca Cin Cout Figure 11. Parasitic Capacitances of the Amplifier RS 1 2 LS CS 1 2 CO 1 Re Xe 2 NOTE: Values are supplied by crystal manufacturer (parallel resonant crystal). Figure 12. Equivalent Crystal Networks RECOMMENDED READING Technical Note TN–24, Statek Corp. Technical Note TN–7, Statek Corp. E. Hafner, “The Piezoelectric Crystal Unit – Definitions and Method of Measurement”, Proc. IEEE, Vol. 57, No. 2 Feb., 1969. D. Kemper, L. Rosine, “Quartz Crystals for Frequency Control”, Electro–Technology, June, 1969. P. J. Ottowitz, “A Guide to Crystal Selection”, Electronic Design, May, 1966. Table 1. Partial List of Crystal Manufacturers Name United States Crystal Corp. Crystek Crystal Statek Corp. Address 3605 McCart Ave., Ft. Worth, TX 76110 2351 Crystal Dr., Ft. Myers, FL 33907 512 N. Main St., Orange, CA 92668 Phone (817) 921–3013 (813) 936–2109 (714) 639–7810 NOTE: Motorola cannot recommend one supplier over another and in no way suggests that this is a complete listing of crystal manufacturers. MOTOROLA MC145149 9 DUAL–MODULUS PRESCALING OVERVIEW The technique of dual–modulus prescaling is well established as a method of achieving high performance frequency synthesizer operation at high frequencies. Basically, the approach allows relatively low–frequency programmable counters to be used as high–frequency programmable counters with speed capability of several hundred MHz. This is possible without the sacrifice in system resolution and performance that results if a fixed (single–modulus) divider is used for the prescaler. In dual–modulus prescaling, the lower speed counters must be uniquely configured. Special control logic is necessary to select the divide value P or P + 1 in the prescaler for the required amount of time (see modulus control definition). Motorola’s dual–modulus frequency synthesizers contain this feature and can be used with a variety of dual– modulus prescalers to allow speed, complexity, and cost to be tailored to the system requirements. Prescalers having P, P + 1 divide values in the range of ÷ 3/÷ 4 to ÷ 128/÷ 129 can be controlled by most Motorola frequency synthesizers. Several dual–modulus prescaler approaches suitable for use with the MC145149 are: MC12009 MC12011 MC12013 MC12015 MC12016 MC12017 MC12018 MC12022A MC12032A ÷ 5/÷ 6 ÷ 8/÷ 9 ÷ 10 / ÷ 11 ÷ 32 / ÷ 33 ÷ 40 / ÷ 41 ÷ 64 / ÷ 65 ÷ 128 / ÷ 129 ÷ 64 / 65 or ÷ 128 / 129 ÷ 64 / 65 or ÷ 128 / 129 440 MHz 500 MHz 500 MHz 225 MHz 225 MHz 225 MHz 520 MHz 1.1 GHz 2.0 GHz DESIGN GUIDELINES The system total divide value, Ntotal (NT) will be dictated by the application, i.e., NT = NTmax = Nmax P + Amax To maximize system frequency capability, the dual–modulus prescaler output must go from low to high after each group of P or P + 1 input cycles. The prescaler should divide by P when its modulus control line is high and by P + 1 when its modulus control is low. For the maximum frequency into the prescaler (fVCO max), the value used for P must be large enough such that: 1. fVCO max divided by P may not exceed the frequency capability of fin (input to the ÷ N and ÷ A counters). 2. The period of fVCO divided by P must be greater than the sum of the times: a. Propagation delay through the dual–modulus prescaler. b. Prescaler setup or release time relative to its modulus control signal. c. Propagation time from fin to the modulus control output for the frequency synthesizer device. A sometimes useful simplification in the programming code can be achieved by choosing the values for P of 8, 16, 32, or 64. For these cases, the desired value of NT results when NT in binary is used as the program code to the ÷ N and ÷ A counters treated in the following manner: 1. Assume the ÷ A counter contains “a” bits where 2a ≥ P. 2. Always program all higher order ÷ A counter bits above “a” to 0. 3. Assume the ÷ N counter and the ÷ A counter (with all the higher order bits above “a” ignored) combined into a single binary counter of n + a bits in length (n = number of divider stages in the ÷ N counter). The MSB of this “hypothetical” counter is to correspond to the MSB of ÷ N and the LSB is to correspond to the LSB of ÷ A. The system divide value, NT, now results when the value of NT in binary is used to program the “new” n + a bit counter. By using the two devices, several dual–modulus values are achievable. MC frequency into the prescaler =NP+A frequency into the phase detector N is the number programmed into the ÷ N counter, A is the number programmed into the ÷ A counter, P and P + 1 are the two selectable divide ratios available in the dual–modulus prescalers. To have a range of NT values in sequence, the ÷ A counter is programmed from 0 through P – 1 for a particular value N in the ÷ N counter. N is then incremented to N + 1 and the ÷ A is sequenced from 0 through P – 1 again. There are minimum and maximum values that can be achieved for NT. These values are a function of P and the size of the ÷ N and ÷ A counters. The constraint N ≥ A always applies. If Amax = P – 1, then Nmin ≥ P – 1. Then NTmin = (P – 1) P + A or (P – 1) P since A is free to assume the value of 0. MC145149 10 DEVICE A DEVICE B DEVICE B DEVICE A MC12009 MC10131 ÷ 20/÷ 21 MC12011 MC12013 ÷ 32/÷ 33 ÷ 40/÷ 41 MC10138 ÷ 50/÷ 51 ÷ 80/÷ 81 ÷ 100/÷ 101 ÷ 40/÷ 41 OR ÷ 80/÷ 81 ÷ 64/÷ 65 OR ÷ 128/÷ 129 ÷ 80/÷ 81 MC10154 NOTE: MC12009, MC12011, and MC12013 are pin equivalent. MC12015, MC12016, and MC12017 are pin equivalent. MOTOROLA PACKAGE DIMENSIONS P SUFFIX PLASTIC DIP CASE 738–03 -A20 11 1 10 NOTES: 1. DIMENSIONING AND TOLERANCING PER ANSI Y14.5M, 1982. 2. CONTROLLING DIMENSION: INCH. 3. DIMENSION L TO CENTER OF LEAD WHEN FORMED PARALLEL. 4. DIMENSION B DOES NOT INCLUDE MOLD FLASH. B C -T- L DIM A B C D E F G J K L M N K SEATING PLANE M E G N F J 20 PL 0.25 (0.010) D 20 PL 0.25 (0.010) M T A M T B M M INCHES MIN MAX 1.010 1.070 0.240 0.260 0.150 0.180 0.015 0.022 0.050 BSC 0.050 0.070 0.100 BSC 0.008 0.015 0.110 0.140 0.300 BSC 15° 0° 0.020 0.040 MILLIMETERS MIN MAX 25.66 27.17 6.10 6.60 3.81 4.57 0.39 0.55 1.27 BSC 1.27 1.77 2.54 BSC 0.21 0.38 2.80 3.55 7.62 BSC 0° 15° 1.01 0.51 D SUFFIX SOG PACKAGE CASE 751D–04 NOTES: 1. DIMENSIONING AND TOLERANCING PER ANSI Y14.5M, 1982. 2. CONTROLLING DIMENSION: MILLIMETER. 3. DIMENSIONS A AND B DO NOT INCLUDE MOLD PROTRUSION. 4. MAXIMUM MOLD PROTRUSION 0.150 (0.006) PER SIDE. 5. DIMENSION D DOES NOT INCLUDE DAMBAR PROTRUSION. ALLOWABLE DAMBAR PROTRUSION SHALL BE 0.13 (0.005) TOTAL IN EXCESS OF D DIMENSION AT MAXIMUM MATERIAL CONDITION. –A– 20 11 –B– 10X P 0.010 (0.25) 1 M B M 10 20X D 0.010 (0.25) M T A B S J S F R C –T– 18X MOTOROLA G K SEATING PLANE X 45 _ DIM A B C D F G J K M P R MILLIMETERS MIN MAX 12.65 12.95 7.40 7.60 2.35 2.65 0.35 0.49 0.50 0.90 1.27 BSC 0.25 0.32 0.10 0.25 0_ 7_ 10.05 10.55 0.25 0.75 INCHES MIN MAX 0.499 0.510 0.292 0.299 0.093 0.104 0.014 0.019 0.020 0.035 0.050 BSC 0.010 0.012 0.004 0.009 0_ 7_ 0.395 0.415 0.010 0.029 M MC145149 11 Motorola reserves the right to make changes without further notice to any products herein. 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