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PCK12429BD 数据表(PDF) 9 Page - NXP Semiconductors |
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PCK12429BD 数据表(HTML) 9 Page - NXP Semiconductors |
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9 / 14 page ![]() Philips Semiconductors Product data PCK12429 25–400 MHz differential PECL clock generator 2002 Jun 03 9 Power supply filtering The PCK12429 is a mixed analog/digital product and as such it exhibits some sensitivities that would not necessarily be seen on a fully digital product. Analog circuitry is naturally susceptible to random noise, especially if this noise is seen on the power supply pins. The PCK12429 provides separate power supplies for the digital circuitry (VCC) and the internal PLL (PLL_VCC) of the device. The purpose of this design technique is to try and isolate the high switching noise digital outputs from the relatively sensitive internal analog phase-locked loop. In a controlled environment such as an evaluation board, this level of isolation is sufficient. However, in a digital system environment where it is more difficult to minimize noise on the power supplies, a second level of isolation may be required. The simplest form of isolation is a power supply filter on the PLL_VCC pin for the PCK12429. Figure 3 illustrates a typical power supply filter scheme. The PCK12429 is most susceptible to noise with spectral content in the 1 kHz to 2 MHz range. A good choice of pole placement should be close to 32 kHz. Therefore the filter should be designed to target this range. The key parameter that needs to be met in the final filter design is the DC voltage drop that will be seen between the VCC supply and the PLL_VCC pin of the PCK12429. From the data sheet the IPLL_VCC current (the current sourced through the PLL_VCC pin) is typically 15 mA (20 mA maximum), assuming that a minimum of 3.0 V must be maintained on the PLL_VCC pin, very little DC voltage drop can be tolerated when a 3.3 V VCC supply is used. The resistor shown in Figure 3 must have a resistance of 10–15 Ω to meet the voltage drop criteria. The RC filter pictured will provide a broadband filter with approximately 100:1 attenuation for noise whose spectral content is above 20 kHz. As the noise frequency crosses the series resonant point of an individual capacitor, its overall impedance begins to look inductive and thus increases with increasing frequency. The parallel capacitor combination shown ensures that a low impedance path to ground exists for frequencies well above the bandwidth of the PLL. VCC SW00745 PLL_VCC PCK12429 0.01 µF 22 µF RS = 10–15 Ω L = 1000 µH R = 15 Ω 3.3 V 3.3 V Figure 3. Power supply filter A higher level of attenuation can be achieved by replacing the resistor with an appropriate valued inductor. Figure 3 shows a 1000 µH choke, this value choke will show a significant impedance at 10 KHz frequencies and above. Because of the current draw and the voltage that must be maintained on the PLL_VCC pin, a low DC resistance inductor is required (less than 15 Ω). Generally the resistor/capacitor filter will be cheaper, easier to implement, and provide an adequate level of supply filtering. The PCK12429 provides sub-nanosecond output edge rates, and thus a good power supply bypassing scheme is a must. Figure 4 shows a representative board layout for the PCK12429. There exists many different potential board layouts and the one pictured is but one. The important aspect of the layout in Figure 4 is the low impedance connections between VCC and GND for the bypass capacitors. Combining good quality general purpose chip capacitors with good PCB layout techniques will produce effective capacitor resonances at frequencies adequate to supply the instantaneous switching current for the PCK12429 outputs. It is imperative that low inductance chip capacitors are used; it is equally important that the board layout does not introduce back all of the inductance saved by using the leadless capacitors. Thin interconnect traces between the capacitor and the power plane should be avoided and multiple large vias should be used to tie the capacitors to the buried power planes. Fat interconnect and large vias will help to minimize layout induced inductance and thus maximize the series resonant point of the bypass capacitors. SW00746 Xtal 1 C3 C2 = VCC = GND = Via C1 C1 R1 = 10–15 Ω C1 = 0.01 µF C2 = 22 µF C3 = 0.1 µF R1 Figure 4. PCB board layout for PCK12429 Note the dotted lines circling the crystal oscillator connection to the device. The oscillator is a series resonant circuit and the voltage amplitude across the crystal is relatively small. It is imperative that no actively switching signals cross under the crystal, as crosstalk energy coupled to these lines could significantly impact the jitter of the device. Special attention should be paid to the layout of the crystal to ensure a stable, jitter free interface between the crystal and the on-board oscillator. Although the PCK12429 has several design features to minimize the susceptibility to power supply noise (isolated power and grounds and fully differential PLL) there still may be applications in which overall performance is being degraded due to system power supply noise. The power supply filter and bypass schemes discussed in this section should be adequate to eliminate power supply noise related problems in most designs. |
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