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ADP3412 Datasheet(PDF) 6 Page - Analog Devices

Part # ADP3412
Description  Dual MOSFET Driver with Bootstrapping
PDF  8 Pages
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Manufacturer  AD [Analog Devices]
Direct Link  http://www.analog.com
Logo AD - Analog Devices

ADP3412 Datasheet(HTML) 6 Page - Analog Devices

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ADP3412
–6–
REV. 0
THEORY OF OPERATION
The ADP3412 is a dual MOSFET driver optimized for driving
two N-channel MOSFETs in a synchronous buck converter
topology. A single PWM input signal is all that is required to
properly drive the high-side and the low-side FETs. Each driver
is capable of driving a 3 nF load with only a 20 ns transition time.
A more detailed description of the ADP3412 and its features
follows. Refer to the general application circuit in Figure 1.
Low-Side Driver
The low-side driver is designed to drive low-RDS(ON) N-channel
MOSFETs. The maximum output resistance for the driver is
5
Ω for both sourcing and sinking gate current. The low output
resistance allows the driver to have 20 ns rise and fall times into
a 3 nF load. The bias to the low-side driver is internally con-
nected to the VCC supply and PGND.
The driver’s output is 180 degrees out of phase with the PWM
input.
High-Side Driver
The high-side driver is designed to drive a floating low RDS(ON)
N-channel MOSFET. The maximum output resistance for the
driver is 5
Ω for both sourcing and sinking gate current. The
low output resistance allows the driver to have 20 ns rise and fall
times into a 3 nF load. The bias voltage for the high-side driver
is developed by an external bootstrap supply circuit, which is
connected between the BST and SW pins.
The bootstrap circuit comprises a diode, D1, and bootstrap
capacitor, CBST. When the ADP3412 is starting up, the SW pin
is at ground, so the bootstrap capacitor will charge up to VCC
through D1. When the PWM input goes high, the high-side
driver will begin to turn ON the high-side MOSFET, Q1, by
pulling charge out of CBST. As Q1 turns ON, the SW pin will
rise up to VIN, forcing the BST pin to VIN + VC(BST), which is
enough gate-to-source voltage to hold Q1 ON. To complete the
cycle, Q1 is switched OFF by pulling the gate down to the volt-
age at the SW pin. When the low-side MOSFET, Q2, turns
ON, the SW pin is pulled to ground. This allows the bootstrap
capacitor to charge up to VCC again. The high-side driver’s
output is in phase with the PWM input.
Overlap Protection Circuit
The Overlap Protection Circuit (OPC) prevents both of the
main power switches, Q1 and Q2, from being ON at the same
time. This is done to prevent shoot-through currents from flow-
ing through both power switches and the associated losses that
can occur during their ON-OFF transitions. The Overlap Pro-
tection Circuit accomplishes this by adaptively controlling the
delay from Q1’s turn OFF to Q2’s turn ON, and by externally
setting the delay from Q2’s turn OFF to Q1’s turn ON.
To prevent the overlap of the gate drives during Q1’s turn OFF
and Q2’s turn ON, the overlap circuit monitors the voltage at
the SW pin. When the PWM input signal goes low, Q1 will begin
to turn OFF (after a propagation delay), but before Q2 can turn
ON, the overlap protection circuit waits for the voltage at the SW
pin to fall from VIN to 1 V. Once the voltage on the SW pin has
fallen to 1 V, Q2 will begin turn ON. By waiting for the voltage
on the SW pin to reach 1 V, the overlap protection circuit ensures
that Q1 is OFF before Q2 turns on, regardless of variations in
temperature, supply voltage, gate charge, and drive current.
To prevent the overlap of the gate drives during Q2’s turn OFF
and Q1’s turn ON, the overlap circuit provides a programmable
delay that is set by a capacitor on the DLY pin. When the PWM
input signal goes high, Q2 will begin to turn OFF (after a propa-
gation delay), but before Q1 can turn ON the overlap protection
circuit waits for the voltage at DRVL to drop to around 10% of
VCC. Once the voltage at DRVL has reached the 10% point,
the overlap protection circuit will wait for a 20 ns typical propa-
gation delay plus an additional delay based on the external
capacitor, CDLY. The delay capacitor adds an additional 1 ns/pF
of delay. Once the programmable delay period has expired, Q1
will begin turn ON. The delay allows time for current to com-
mutate from the body diode of Q2 to an external Schottky diode,
which allows turnoff losses to be reduced. Although not as fool-
proof as the adaptive delay, the programmable delay adds a
safety margin to account for variations in size, gate charge, and
internal delay of the external power MOSFETs.
APPLICATION INFORMATION
Supply Capacitor Selection
For the supply input (VCC) of the ADP3412, a local bypass
capacitor is recommended to reduce the noise and to supply some
of the peak currents drawn. Use a 1
µF, low ESR capacitor.
Multilayer ceramic chip (MLCC) capacitors provide the best
combination of low ESR and small size and can be obtained from
the following vendors:
Murata
GRM235Y5V106Z16
www.murata.com
Taiyo-
Yuden
EMK325F106ZF
www.t-yuden.com
Tokin
C23Y5V1C106ZP
www.tokin.com
Keep the ceramic capacitor as close as possible to the ADP3412.
Bootstrap Circuit
The bootstrap circuit uses a charge storage capacitor (CBST) and
a Schottky diode, as shown in Figure 1. Selection of these com-
ponents can be done after the high-side MOSFET has been
chosen.
The bootstrap capacitor must have a voltage rating that is able
to handle the maximum battery voltage plus 5 volts. A minimum
50 V rating is recommended. The capacitance is determined
using the following equation:
C
Q
V
BST
GATE
BST
=
∆
where, QGATE is the total gate charge of the high-side MOSFET,
and
∆V
BST is the voltage droop allowed on the high-side MOSFET
drive. For example, the IRF7811 has a total gate charge of about
20 nC. For an allowed droop of 200 mV, the required boot-
strap capacitance is 100 nF. A good quality ceramic capacitor
should be used.
A Schottky diode is recommended for the bootstrap diode due
to its low forward drop, which maximizes the drive available for
the high-side MOSFET. The bootstrap diode must have a mini-
mum 40 V rating to withstand the maximum battery voltage
plus 5 V. The average forward current can be estimated by:
MAX
GATE
F(AVG)
f
Q
I
×
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