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A8650 Datasheet(PDF) 25 Page - Allegro MicroSystems |
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A8650 Datasheet(HTML) 25 Page - Allegro MicroSystems |
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25 / 31 page ![]() Low Input Voltage, Adjustable Frequency 2 A Synchronous Buck Regulator with EN/SYNC and Power OK A8650 25 Allegro MicroSystems, LLC 115 Northeast Cutoff Worcester, Massachusetts 01615-0036 U.S.A. 1.508.853.5000; www.allegromicro.com 5. Calculate the frequency of the ESR zero (fZ1) formed by the output capacitor(s). Use equation 23 (repeated here): = fZ1 COUT ESR × × 2� 1 If fZ1 is at least one decade higher than the target crossover frequency (fC) then fZ1 can be ignored. This is usually the case for a design using ceramic output capacitors. Use equation 27 to calculate the value of CP by setting fP3 to either 5 × fC or fSW / 2, whichever is higher. Alternatively, if fZ1 is near or below the target crossover fre- quency (fC), then use equation 27 to calculate the value of CP by setting fP3 equal to fZ1. This is usually the case for a design using high ESR electrolytic output capacitors. Power Dissipation and Thermal Calculations The power dissipated in the A8650 is the sum of the power dis- sipated from the VIN supply current (PIN), the power dissipated due to the switching of the internal power high-side MOSFET (PSW1), the power dissipated due to the rms current being conducted by the high- and low-side MOSFETs (PCOND1 and PCOND2), the power dissipated by the low-side MOSFET body diode during the non-overlap times, and the power dissipated by the internal gate drivers (PDRIVER1 and PDRIVER2). The power dissipated from the VIN supply current can be calcu- lated using the following equation: PIN = VIN × IQ + (VIN – VGS) × (QG1 + QG2 ) × fSW (30) where VIN is the input voltage, IQ is the input quiescent current drawn by the A8650 (nominally 2 mA), VGS is the MOSFET gate drive voltage, typically 5.0 V, QG1 and QG2 are the internal high- and low-side MOSFET gate charges (approximately 3.3 nC and 1.4 nC respectively), and fSW is the PWM switching frequency. The switching losses dissipated by the internal high-side MOSFET during PWM switching can be calculated using the following equation: = PSW1 VIN IOUT fSW (tr + tf ) × × × 2 (31) where VIN is the input voltage, IOUT is the output current, fSW is the PWM switching frequency, and tr and tf are the rise and fall times measured at the SW node. Approximate values for tr range from 10 to 15 ns. The fall time is usually about 50% faster than the rise time. The conduction losses dissipated by the high-side MOSFET while it is conducting can be calculated using the following equation: = PCOND1 Irms(FET) RDS(on)HS VOUT VIN × × + 12 2 ∆IL2 IOUT 2 = RDS(on)HS × (32) where IOUT is the regulator output current, ΔIL is the peak-to-peak inductor ripple current, and RDS(on)HS is the on-resistance of the high-side MOSFET. The conduction losses dissipated by the low-side MOSFET while it is conducting can be calculated using the following equation: = PCOND2 Irms(FET) RDS(on)LS VOUT VIN × × + – 12 2 ∆IL2 IOUT 1 2 = RDS(on)LS × (33) where IOUT is the regulator output current, ΔIL is the peak-to-peak inductor ripple current, and RDS(on)LS is the on-resistance of the low-side MOSFET. The RDS(on)of the MOSFETs has some initial tolerance plus an increase from self-heating and elevated ambient temperatures. A conservative design should accommodate an RDS(on) with at least a 15% initial tolerance plus 0.39%/°C increase due to temperature. |
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