MS2258: Reducing the Size and Complexity of an Isolated Synchronous Gate Driver

Technical Article
MS-2258
.
Reducing the Size and
Complexity of an Isolated
Synchronous Gate Driver
driver IC may be needed. Another point to consider and a
major disadvantage of pulse transformers in gate driver
applications is that they do not handle well signals that have
more than 50% duty cycle. This is due to the fact that
transformers can deliver only ac signals because the core flux
must be reset each half cycle in order to maintain a voltsecond balance.
By Brian Kennedy, Senior Applications Engineer,
Digital Isolator Group, Analog Devices, Inc.
IDEA IN BRIEF
The traditional approach to designing an isolated dc-to-dc
converter with synchronous rectification involves using
optocouplers or pulse transformers for isolation and mating
them together with a gate driver IC. This article will illustrate
the limitations of optocouplers and pulse transformers and
present a more integrated approach, which has higher
performance and a much smaller solution size and cost.
PULSE TRANSFORMERS
Using pulse transformers to couple low level signals, isolate
them, and drive power switches offers advantages, but it
comes with some limitations. An advantage of the pulse
transformer in gate drive applications is the pulse transformer
can be used to step up from 3 V or 5 V logic level to the
higher level voltages of 15 V or more needed to drive the
gate of a MOSFET. Unfortunately, to drive high current
synchronous rectifier circuits, a separate high current gate
Another disadvantage of the pulse transformer is the
efficiency loss. When a pulse transformer is used to drive the
gate of a MOSFET, the transformer must be driven in a
positive level, followed by a negative level, to maintain a voltsecond balance. The energy used to drive to a negative level
is not used to drive the gate of the MOSFET; the gate is
charged only by the positive voltage level. For the typical
application where the transformer is driven by a positive dc
voltage, a dc blocking capacitor is connected to the
transformer input, and the transformer is driven by a
positive voltage that is ½ the applied voltage. That means
the negative voltage is also ½ the applied voltage, so that the
efficiency of the pulse transformer is reduced to 50%. If a
gate driver is added to the transformer output, the overall
efficiency of the transformer and gate driver will no longer
be 50%, but there will still be at least 50% efficiency loss in
the pulse transformer alone.
It has been shown here that the pulse transformer in a gate
driver application has disadvantages of duty cycle limitation,
poor efficiency, and larger solution size, which make it
undesirable for high power, high density synchronous
rectification applications.
Figure 1. Pulse Transformer, Optocoupler, and ADuM3220 Gate Driver Solutions
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MS-2258
Technical Article
OPTOCOUPLERS
ADUM3220 4 A GATE DRIVER
Using optocouplers as a gate driver for synchronous
rectification can offer some advantages over pulse
transformers, but the use of the optocoupler comes with its
own challenges. The optocoupler does not need to maintain
a volt-second balance like the pulse transformer does, so it
does not have the same limitation on duty cycle that the
pulse transformer has. But the speed of response of the
optocoupler is limited due to the capacitance (60 pF typical)
of the primary side light emitting diode (LED), and driving
the diode to speeds up to 1 MHz can be limited by its
propagation delay (100 ns max) and slow rise and fall time
(30 ns max).
The ADuM3220 was designed to be used as a 4A gate driver
in an isolated system for synchronous dc-to-dc conversion.
Traditional solutions have used two isolators and a dual gate
driver. As shown in Figure 1, a dual gate driver IC can be
mated with two pulse transformers or two optocoupler
channels to provide a fairly large solution size. Given that
power supply applications require large amounts of power in
a small area, the ADuM3220, as shown in Figure 1, is a
solution that is more than 50% smaller and is a more
integrated solution for lower cost.
A main issue with using optocouplers for synchronous
rectifier applications is the amount of variation in the timing
between channels. Optocouplers are built as discrete devices
in a plastic package, and the variation from channel to
channel cannot be controlled like they can be in an
integrated semiconductor process, so the channel to channel
matching can be large (40 ns max). In a synchronous
rectification circuit, the timing between channels needs to be
tightly controlled to help reduce the dead time between one
channel turning off and another channel turning on,
otherwise the efficiency will suffer as the switching losses
increase.
Designing with optocouplers can be challenging, due to the
nature of the current transfer ratio (CTR), which defines the
ratio of the amount of current that is seen at the output
transistor over the amount of current that is needed to drive
the LED. The CTR is affected by temperature and aging, so
the designer needs to estimate the change in CTR over the
lifetime and temperature range of the optocoupler. To
maintain the CTR over operation conditions, the current
needed to drive the LED can be more than 10 mA, which
may be too much power dissipation for high efficiency
designs.
In addition, resistors are needed to bias the LED and
phototransistors, and a gate driver IC is needed to deliver the
high peak currents that the optocoupler can’t provide for
high power synchronous rectifier supplies. For compact state
of the art power supplies, the optocoupler solution size will
become prohibitively large.
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Synchronous rectification uses N-channel MOSFETs instead
of diodes to reduce the conduction losses and increase
efficiency in power supplies where many amperes of current
are to be delivered. Implementing the synchronous dc-to-dc
converter architecture requires synchronizing the switching
of the secondary MOSFET switches with the primary
MOSFET switches. Figure 2 illustrates the ADuM3220
application circuit for an isolated synchronous dc-to-dc
converter with unregulated output voltage.
The dc-to-dc controller sends the PWM drive signals to the
primary and secondary switches. Primary switches Q1 and
Q2 are turned on in a push-pull action with a break before
make timing to drive the two primary coils of the transformer
T1, as shown in Figure 2 timing waveforms. The secondary
coil of T1 needs to be switched in sync with the primary
coils by switching on Q3 when turning on Q1, and turning
on Q4 when turning on Q2. Note, Q3’ and Q4’ PWM
waveforms, if they were shown, would be advanced in time
by the known propagation delay of the ADuM3220 so that
Q3 and Q4 appear in time as they should. The ADuM3220
has a typical propagation delay of only 45 ns, which includes
the digital isolator delay and the gate driver delay. By
integrating the gate driver with the isolator, the specification
of propagation delay is more precise, an advantage over
discrete pulse transformer and optocoupler solutions.
When PWM switching is performed at a high frequency, the
PWM control signals need very tight control. For example,
when the PWM frequency is at the ADuM3220 maximum
switching frequency of 1 MHz and a duty cycle of 50% is
used, the pulse width is at 500 ns. At this small pulse width,
the matching between channels of the ADuM3220 needs to
be very good to deliver precise switching. The ADuM3220
has a typical channel-to-channel matching of 1 ns, with a
maximum of 5 ns over temperature. This precise matching
between channels of the ADuM3220 helps to prevent cross
December 2011 | Page 2 of 4
Technical Article
MS-2258
conduction and protects the MOSFETs from damage, as well
as allowing the minimum amount of dead time, to reduce
switching losses and improve efficiency.
Next, we will consider applications where an isolated
feedback is used to tightly control the output voltage, and the
duty cycle will not be a fixed 50% but will vary to control the
output voltage. In these applications, during the time that
the primary switches are both off, it may be desired to allow
the Q3 and Q4 switches to be on at the same time to prevent
the body diodes of Q3 and Q4 from conducting, which
would be less efficient. The application circuit for the
ADuM3221 that is shown in Figure 3 is a 4 A gate driver that
is just like the ADuM3220 but does not have the nonoverlap
control logic, allowing Q3 and Q4 to be on at the same time.
Unlike the ADuM3220, the timing diagram for the
ADuM3221 gate driver with regulated output shown in
Figure 3 can allow the switches Q3 and Q4 to conduct when
Q1 and Q2 are both off.
In summary, for isolated synchronous dc-to-dc applications,
the ADuM3220/ADuM3221 have been shown to reduce the
solution size by more than 50%, reduce the complexity of
design through integration, and provide much improved
timing performance over pulse transformer and optocoupler
solutions.
Figure 2. ADuM3220 Application Schematic and Timing Waveforms
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MS-2258
Technical Article
Figure 3. ADuM3221 Application Schematic with Regulated Output and Timing Waveforms
RESOURCES
ABOUT THE AUTHOR
For more information on digital isolators, visit
www.analog.com/iCoupler.
Brian Kennedy is an applications
engineer for the Digital Isolator
Products Team at Analog Devices.
Brian holds a BSEE from SUNY
Buffalo, NY, and has extensive
experience in applications of
digital isolator ICs. He is currently
responsible for power supply and
industrial applications in the digital
isolation group.
Products Mentioned in This Article
Product
ADuM3220
ADuM3221
Description
Isolated 4 A Dual-Channel Gate Driver
Isolated 4 A Dual-Channel Gate Driver
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