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MC145151P2 Datasheet(PDF) 28 Page - Motorola, Inc |
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MC145151P2 Datasheet(HTML) 28 Page - Motorola, Inc |
28 / 36 page MC145151–2 through MC145158–2 MOTOROLA 28 DESIGN CONSIDERATIONS PHASE–LOCKED LOOP — LOW–PASS FILTER DESIGN C) _ + A C R2 C VCO C VCO R2 B) A) C VCO PDout PDout φR — φV — PDout — φR φV R1 R1 R1 R1 R2 NOTE: Sometimes R1 is split into two series resistors, each R1 ÷ 2. A capacitor CC is then placed from the midpoint to ground to further filter φV and φR. The value of CC should be such that the corner frequency of this network does not significantly affect ωn. The φR and φV outputs swing rail–to–rail. Therefore, the user should be careful not to exceed the common mode input range of the op amp used in the combiner/loop filter. DEFINITIONS: N = Total Division Ratio in feedback loop K φ (Phase Detector Gain) = VDD/4π for PDout K φ (Phase Detector Gain) = VDD/2π for φV and φR KVCO (VCO Gain) = 2 π∆fVCO ∆VVCO for a typical design wn (Natural Frequency) ≈ 2 πfr 10 (at phase detector input). 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. φR — φV — F(s) = ASSUMING GAIN A IS VERY LARGE, THEN: F(s) = ζ = ωn = NR1C R1sC + 1 ωn = ζ = ωnR2C 2 R2sC + 1 R1sC 1 N ωn 2K φKVCO F(s) = ζ = ωn = (R1 + R2)sC + 1 R2sC + 1 NC(R1 + R2) R2C + N K φKVCO K φKVCO NCR1 0.5 ωn K φKVCO K φKVCO |
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