Adjustable Frequency Buck or Buck-Boost Pre-Regulator with a
Synchronous Buck, 3 Internal LDOs, Watchdog Timer, NPOR, and FF0/FF1
A4408
38
Allegro MicroSystems, LLC
955 Perimeter Road
Manchester, NH 03103-3353 U.S.A.
www.allegromicro.com
from its nominal value until the error amplifier can bring the
output voltage back to its nominal value. The speed at which the
error amplifier will bring the output voltage back to its setpoint
will depend mainly on the closed-loop bandwidth of the system.
Selection of the compensation components (RZ1, CZ1, CP1) are
discussed in more detail in the Pre-Regulator Compensation sec-
tion of this datasheet.
The output voltage ripple (ΔVVREG) is a function of the output
capacitors parameters: COUT, ESRCo, and ESLCo according to
equation 8.
(8)
V=I× ESR+
VREG LCo
VIN VREG
× ESL+
Co
L
ΔΔ
The type of output capacitors will determine which terms of
equation 8 are dominant. For the A4408 and automotive environ-
ments, only ceramic capacitors are recommended. The ESRCO
and ESLCO of ceramic capacitors are virtually zero, so the peak-
to-peak output voltage ripple of VVREG will be dominated by the
third term of equation 8.
L
(9)
ΔVVREG(PP)=
Pre-Regulator Ceramic Input Capacitance
The ceramic input capacitors must limit the voltage ripple at the
VIN pin to a relatively low voltage during maximum load. Equa-
tion 10 can be used to calculate the minimum input capacitance,
VREG(MAX)
(10)
CIN ≥
where IVREG(MAX) is the maximum current from the pre-regulator,
(11)
I= I+ +
VREG(MAX)V5 V5P 3V3
II+
OUT(ADJ) OUT(ADJ)
+ 20 mA
A good design should consider the DC bias effect on a ceramic
capacitor—as the applied voltage approaches the rated value, the
capacitance value decreases. The X7R-type capacitors should be
the primary choices due to their stability versus both DC bias and
temperature. For all ceramic capacitors, the DC bias effect is even
more pronounced on smaller case sizes, so a good design will use
the largest affordable case size (i.e. 1206/16 V or 1210/50 V).
Also, for improved EMI/EMC performance, it is recommended
that two small capacitors be placed as close as physically possible
to the VIN pins to address frequencies above 10 MHz. For exam-
ple, a 0.1 µF/X7R/0603 and a 220 pF/COG/0402 capacitor will
address frequencies up to 20 MHz and 200 MHz, respectively.
Pre-Regulator Asynchronous Diode (D1)
The highest peak current in the asynchronous diode (D1) occurs
during overload and is limited by the A4408. Equation 4 can be
used to calculate this current.
The highest average current in the asynchronous diode occurs
when VVIN is at its maximum, DBOOST = 0%, and DBUCK = mini-
mum (10%),
IAVG = (1 – DBUCK) × IVREG(MAX) = 0.9 × IVREG(MAX) (12)
where IVREG(MAX) is calculated using equation 11.
Pre-Regulator Boost MOSFET (Q1)
The maximum RMS current in the boost MOSFET (Q1) occurs
when VVIN is very low and the boost operates at its maximum
duty cycle,
(13)
I=
Q1(RMS) D×
MAX(BST) I–
PEAK1
ΔIL1 ΔIL1
2
+
where IPEAK1 and ΔIL1 are derived using equations 4 and 5,
respectively, and DMAX(BST) is identified in the Electrical Charac-
teristics table.
The boost MOSFET should have a total gate charge of less than
14 nC at a VGS of 5 V. The VDS rating of the boost MOSFET
should be at least 20 V. Several recommended part numbers are
shown in the Functional Block Diagram / Typical Schematic.
Pre-Regulator Boost Diode (D2)
In buck mode, the maximum average current in this diode is simply
the output current, calculated with equation 11. However, in buck-
boost mode, the peak currents in this diode may increase signifi-
cantly. The A4408 will limit the current to the value calculated by
equation 4.
Pre-Regulator Soft-Start and Hiccup Timing
(CSS1)
The soft-start time of the pre-regulator is determined by the value
of the capacitance at the soft-start pin (CSS1).
If the A4408 is starting into a very heavy load, a very fast soft-
start time may cause the regulator to exceed the pulse-by-pulse
overcurrent threshold. This occurs because the total of the full
load current, the inductor ripple current, and the additional cur-
rent required to charge the output capacitors (IC(OUT) = COUT ×
VOUT / tSS) is higher than the pulse-by-pulse current threshold, as
shown in Figure 26.