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LTC3727LX-1_15 Datasheet, PDF (14/28 Pages) Linear Technology – High Efficiency, 2-Phase Synchronous Step-Down Switching Regulator
LTC3727LX-1
APPLICATIO S I FOR ATIO
BVDSS specification for the MOSFETs as well; most of the
logic level MOSFETs are limited to 30V or less.
Selection criteria for the power MOSFETs include the
on-resistance RDS(ON), reverse transfer capacitance CRSS,
input voltage and maximum output current. When the
LTC3727LX-1 is operating in continuous mode the duty
cycles for the top and bottom MOSFETs are given by:
Main Switch Duty Cycle = VOUT
VIN
Synchronous Switch Duty Cycle = VIN – VOUT
VIN
The MOSFET power dissipations at maximum output
current are given by:
( ) ( ) PMAIN
=
VOUT
VIN
IMAX
2
1+ δ
RDS(ON) +
k(VIN)2 (IMAX )(CRSS )(f)
( ) ( ) PSYNC
=
VIN
– VOUT
VIN
IMAX
2
1+ δ
RDS(ON)
where δ is the temperature dependency of RDS(ON) and k
is a constant inversely related to the gate drive current.
Both MOSFETs have I2R losses while the topside N-channel
equation includes an additional term for transition losses,
which are highest at high input voltages. For VIN < 20V the
high current efficiency generally improves with larger
MOSFETs, while for VIN > 20V the transition losses rapidly
increase to the point that the use of a higher RDS(ON) device
with lower CRSS actually provides higher efficiency. The
synchronous MOSFET losses are greatest at high input
voltage when the top switch duty factor is low or during a
short-circuit when the synchronous switch is on close to
100% of the period.
The term (1+δ) is generally given for a MOSFET in the form
of a normalized RDS(ON) vs Temperature curve, but
δ = 0.005/°C can be used as an approximation for low
voltage MOSFETs. CRSS is usually specified in the MOS-
FET characteristics. The constant k = 1.7 can be used to
14
estimate the contributions of the two terms in the main
switch dissipation equation.
The Schottky diode D1 shown in Figure 2 conducts during
the dead-time between the conduction of the two power
MOSFETs. This prevents the body diode of the bottom
MOSFET from turning on, storing charge during the dead-
time and requiring a reverse recovery period that could
cost as much as 3% in efficiency at high VIN. A 1A to 3A
Schottky is generally a good compromise for both regions
of operation due to the relatively small average current.
Larger diodes result in additional transition losses due to
their larger junction capacitance. Schottky diodes should
be placed in parallel with the synchronous MOSFETs when
operating in pulse-skip mode or in Burst Mode operation.
CIN and COUT Selection
The selection of CIN is simplified by the multiphase archi-
tecture and its impact on the worst-case RMS current
drawn through the input network (battery/fuse/capacitor).
It can be shown that the worst-case RMS current occurs
when only one controller is operating. The controller with
the highest (VOUT)(IOUT) product needs to be used in the
formula below to determine the maximum RMS current
requirement. Increasing the output current, drawn from
the other out-of-phase controller, will actually decrease
the input RMS ripple current from this maximum value
(see Figure 4). The out-of-phase technique typically re-
duces the input capacitor’s RMS ripple current by a factor
of 30% to 70% when compared to a single phase power
supply solution.
The type of input capacitor, value and ESR rating have
efficiency effects that need to be considered in the selec-
tion process. The capacitance value chosen should be
sufficient to store adequate charge to keep high peak
battery currents down. 22µF to 47µF is usually sufficient
for a 25W output supply operating at 250kHz. The ESR of
the capacitor is important for capacitor power dissipation
as well as overall battery efficiency. All of the power (RMS
ripple current • ESR) not only heats up the capacitor but
wastes power from the battery.
Medium voltage (20V to 35V) ceramic, tantalum, OS-CON
and switcher-rated electrolytic capacitors can be used as
input capacitors, but each has drawbacks: ceramic voltage
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