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ADP3191 Datasheet(PDF) 14 Page - Analog Devices |
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ADP3191 Datasheet(HTML) 14 Page - Analog Devices |
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14 / 28 page ![]() ADP3191 Rev. 0 | Page 14 of 28 APPLICATION INFORMATION The design parameters for a typical Intel VRD 10.1-compliant CPU application are as follows: • Input voltage (VIN) = 12 V • VID setting voltage (VVID) = 1.300 V • Duty cycle (D) = 0.108 • Nominal output voltage at no load (VONL) = 1.281 V • Nominal output voltage at 101 A load (VOFL) = 1.180 V • Static output voltage drop based on a 1.0 mΩ load line (RO) from no load to full load (VD) = VONL − VOFL = 1.281 V − 1.180 V = 101 mV • Maximum output current (IO) = 119 A • Maximum output current step (ΔIO) = 95 A • Number of phases (n) = 4 • Switching frequency per phase (fSW) = 330 kHz SETTING THE CLOCK FREQUENCY The ADP3191/ADP3191A use a fixed-frequency control architecture. The frequency is set by an external timing resistor (RT). The clock frequency and the number of phases determine the switching frequency per phase, which relates directly to switching losses and the sizes of the inductors and/or the input and output capacitors. With n = 4 for four phases, a clock frequency of 1.32 MHz sets the switching frequency (fSW) of each phase to 330 kHz, which represents a practical trade-off between the switching losses and the sizes of the output filter components. Figure 3 shows that to achieve 1.32 MHz oscillator frequency, the correct value for RT is 130 kΩ. Alternatively, the value for RT can be calculated using Ω − × × = k 31 pF 7 . 4 1 SW T f n R (1) where 4.7 pF and 31 kΩ are internal IC component values. For good initial accuracy and frequency stability, a 1% resistor is recommended. SOFT START AND CURRENT-LIMIT LATCH-OFF DELAY TIMES Because the soft start and current-limit latch-off delay functions share the DELAY pin, these two parameters must be considered together. The first step is to set CDLY for the soft start ramp. This ramp is generated with a 20 μA internal current source. The value of RDLY has a second-order impact on the soft start time because it sinks part of the current source to ground. However, as long as RDLY is kept greater than 200 kΩ, this effect is minor. The value for CDLY can be approximated using VID SS DLY VID DLY V t R V C × ⎟ ⎟ ⎠ ⎞ ⎜ ⎜ ⎝ ⎛ × − μ = 2 A 20 (2) where tSS is the desired soft start time. Assuming an RDLY of 390 kΩ and a desired soft start time of 3 ms, CDLY is 36 nF. The closest standard value for CDLY is 39 nF. Once CDLY is chosen, RDLY can be calculated for the current-limit latch-off time using DLY DELAY DLY C t R × = 96 . 1 (3) If the result for RDLY is less than 200 kΩ, a smaller soft start time should be considered by recalculating the equation for CDLY, or a longer latch-off time should be used. RDLY should never be less than 200 kΩ. In this example, a delay time of 9 ms results in RDLY = 452 kΩ. The closest standard 5% value is 470 kΩ. INDUCTOR SELECTION The choice of inductance for the inductor determines the ripple current in the inductor. Less inductance leads to more ripple current, which increases the output ripple voltage and conduction losses in the MOSFETs. But it also allows using smaller inductors and, for a specified peak-to-peak transient deviation, less total output capacitance. Conversely, a higher inductance means lower ripple current and reduced conduction losses but requires larger inductors and more output capacitance for the same peak-to-peak transient deviation. In any multiphase converter, a practical value for the peak-to-peak inductor ripple current is less than 50% of the maximum dc current in the same inductor. Equation 4 shows the relationship between the inductance, oscillator frequency, and peak-to-peak ripple current in the inductor. ( ) L f D V I SW VID R × − × = 1 (4) Equation 5 can be used to determine the minimum inductance based on a given output ripple voltage. ( ) ( ) RIPPLE SW O VID V f D n R V L × × − × × ≥ 1 (5) Solving Equation 5 for a 10 mV p-p output ripple voltage yields ( ) nH 224 mV 10 kHz 330 0.432 1 mΩ 1.0 V 1.3 = × − × × ≥ L If the resulting ripple voltage is less than it was designed for, make the inductor smaller until the ripple value is met. This allows optimal transient response and minimum output decoupling. |
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