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MPC950 датащи(PDF) 7 Page - Motorola, Inc |
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MPC950 датащи(HTML) 7 Page - Motorola, Inc |
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7 / 13 page ![]() MPC950 MPC951 TIMING SOLUTIONS BR1333 — Rev 6 7 MOTOROLA MPC950 Figure 1. Dual Frequency Configuration fsela ‘1’ fselb ‘1’ fselc ‘1’ fseld ‘0’ Input Ref 16.66MHz 66.66MHz Qa 33.33MHz Qb 33.33MHz Qc 1 1 2 MPC950 Figure 2. Dual Frequency Configuration ‘1’ ‘0’ ‘0’ ‘1’ Input Ref 33.33MHz 66.66MHz Qa 66.66MHz Qb 66.66MHz Qc 1 1 2 FBsel ‘0’ FBsel ‘1’ fsela fselb fselc fseld 66.66MHz Qd 5 33.33MHz Qd 5 MPC950 Figure 3. Dual Frequency Configuration fsela ‘1’ fselb ‘1’ fselc ‘1’ fseld ‘1’ Input Ref 16.66MHz 66.66MHz Qa 33.33MHz Qb 33.33MHz Qc 1 1 2 MPC950 Figure 4. Triple Frequency Configuration ‘0’ ‘0’ ‘1’ ‘1’ Input Ref 20MHz 160MHz Qa 80MHz Qb 40MHz Qc 1 1 2 FBsel ‘0’ FBsel ‘0’ fsela fselb fselc fseld 33.33MHz Qd 5 40MHz Qd 5 MPC951 ‘1’ ‘0’ ‘0’ ‘0’ Input Ref 75MHz Ext_FB 1 MPC951 ‘0’ ‘0’ ‘0’ ‘1’ Input Ref 25MHz Ext_FB 1 fsela fselb fselc fseld fsela fselb fselc fseld 75MHz Qa 75MHz Qb 75MHz Qc 1 1 2 75MHz Qd 5 Figure 5. “Zero” Delay Buffer Figure 6. “Zero” Delay Frequency Multiplier 1 100MHz Qa 50MHz Qb 50MHz Qc 1 1 2 25MHz Qd 5 Jitter Performance of the MPC950/951 With the clock rates of today’s digital systems continuing to increase more emphasis is being placed on clock distribution design and management. Among the issues being addressed is system clock jitter and how that affects the overall system timing budget. The MPC950/951 was designed to minimize clock jitter by employing a differential bipolar PLL as well as incorporating numerous power and ground pins in the design. The following few paragraphs will outline the jitter performance of the MPC950/951, illustrate the measurement limitations and provide guidelines to minimize the jitter of the device. The most commonly specified jitter parameter is cycle–to–cycle jitter. Unfortunately with today’s high performance measurement equipment there is no way to measure this parameter for jitter performance in the class demonstrated by the MPC950/951. As a result different methods are used which approximate cycle–to–cycle jitter. The typical method of measuring the jitter is to accumulate a large number of cycles, create a histogram of the edge placements and record peak–to–peak as well as standard deviations of the jitter. Care must be taken that the measured edge is the edge immediately following the trigger edge. If this is not the case the measurement inaccuracy will add significantly to the measured jitter. The oscilloscope cannot collect adjacent pulses, rather it collects data from a very large sample of pulses. It is safe to assume that collecting pulse information in this mode will produce jitter values somewhat larger than if consecutive cycles were measured, therefore, this measurement will represent an upper bound of cycle–to–cycle jitter. Most likely, this is a conservative estimate of the cycle–to–cycle jitter. There are two sources of jitter in a PLL based clock driver, the commonly known random jitter of the PLL and the less intuitive jitter caused by synchronous, different frequency outputs switching. For the case where all of the outputs are |
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