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MAX1540A Datasheet, PDF (40/49 Pages) Maxim Integrated Products – Dual Step-Down Controllers with Saturation Protection, Dynamic Output, and Linear Regulator
Dual Step-Down Controllers with Saturation
Protection, Dynamic Output, and Linear Regulator
Power-MOSFET Dissipation
Worst-case conduction losses occur at the duty factor
extremes. For the high-side MOSFET (NH), the worst-
case power dissipation due to resistance occurs at
minimum input voltage:
PD
(NH
Resistance)
=
⎛
⎝⎜
VOUT
VIN
⎞
⎠⎟
(ILOAD )2
×
RDS(ON)
Generally, use a small high-side MOSFET to reduce
switching losses at high input voltages. However, the
RDS(ON) required to stay within package power-dissi-
pation limits often restricts how small the MOSFET can
be. The optimum occurs when the switching losses
equal the conduction (RDS(ON)) losses. High-side
switching losses do not become an issue until the input
is greater than approximately 15V.
Calculating the power dissipation in high-side
MOSFETs (NH) due to switching losses is difficult, since
it must allow for difficult-to-quantify factors that influ-
ence the turn-on and turn-off times. These factors
include the internal gate resistance, gate charge,
threshold voltage, source inductance, and PC board
layout characteristics. The following switching loss cal-
culation provides only a very rough estimate and is no
substitute for breadboard evaluation, preferably includ-
ing verification using a thermocouple mounted on NH:
( )2
PD (NH Switching) = VIN(MAX)
CRSS × fSW × ILOAD
IGATE
where CRSS is the reverse transfer capacitance of NH,
and IGATE is the peak gate-drive source/sink current
(1A typ).
Switching losses in the high-side MOSFET can become
a heat problem when maximum AC adapter voltages
are applied due to the squared term in the switching-
loss equation (C ✕ VIN2 ✕ fSW). If the high-side MOS-
FET chosen for adequate RDS(ON) at low-battery
voltages becomes extraordinarily hot when subjected
to VIN(MAX), consider choosing another MOSFET with
lower parasitic capacitance.
For the low-side MOSFET (NL), the worst-case power
dissipation always occurs at maximum battery voltage:
PD
(NL
Resistance)
=
⎡
⎢1-
⎣⎢
⎛
⎜
⎝
VOUT
VIN(MAX)
⎞
⎟
⎠
⎤
⎥
⎦⎥
(ILOAD
)2
× RDS(ON)
The absolute worst case for MOSFET power dissipation
occurs under heavy overload conditions that are
greater than ILOAD(MAX) but are not high enough to
exceed the current limit and cause the fault latch to trip.
To protect against this possibility, “overdesign” the cir-
cuit to tolerate:
ILOAD
=
IVALLEY(MAX)
+
⎛
⎝⎜
VOUT (VIN
2VIN
− VOUT
fSW L
)
⎞
⎠⎟
where IVALLEY(MAX) is the maximum valley current
allowed by the current-limit circuit, including threshold
tolerance and sense-resistance variation. The
MOSFETs must have a relatively large heatsink to han-
dle the overload power dissipation.
Choose a Schottky diode (DL) with a forward-voltage
drop low enough to prevent the low-side MOSFET’s
body diode from turning on during the dead time. As a
general rule, select a diode with a DC current rating
equal to 1/3 the load current. This diode is optional and
can be removed if efficiency is not critical.
Applications Information
Step-Down Converter Dropout
Performance
The output-voltage adjustable range for continuous-
conduction operation is restricted by the nonadjustable
minimum off-time one-shot. For best dropout perfor-
mance, use the slower (200kHz) on-time setting. When
working with low input voltages, the duty-factor limit
must be calculated using worst-case values for on- and
off-times. Manufacturing tolerances and internal propa-
gation delays introduce an error to the TON K-factor.
This error is greater at higher frequencies (Table 3).
Also, keep in mind that transient-response performance
of buck regulators operated too close to dropout is
poor, and bulk output capacitance must often be
added (see the VSAG equation in the Design Procedure
section).
The absolute point of dropout is when the inductor cur-
rent ramps down during the minimum off-time (ΔIDOWN)
as much as it ramps up during the on-time (ΔIUP). The
ratio h = ΔIUP/ΔIDOWN indicates the controller’s ability
to slew the inductor current higher in response to
increased load, and must always be greater than 1. As
h approaches 1, the absolute minimum dropout point,
the inductor current cannot increase as much during
each switching cycle, and VSAG greatly increases
unless additional output capacitance is used.
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