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be checked carefully in applications where operation near
dropout is important—like 3.3V to 2.5V converters. Fre-
quencies above 500kHz can cause erratic current limit
operation and are not recommended.
LAYOUT CONSIDERATIONS
Grounding
Proper grounding is critical for the LTC1430A to obtain
specified output regulation. Extremely high peak currents
(as high as several amps) can flow between the bypass
capacitors and the PV
CC1
, PV
CC2
and PGND pins. These
currents can generate significant voltage differences be-
tween two points that are nominally both “ground.” As a
general rule, GND and PGND should be totally separated
on the layout, and should be brought together at only one
point, right at the LTC1430A GND and PGND pins. This
helps minimize internal ground disturbances in the
LTC1430A by keeping PGND and GND at the same poten-
tial, while preventing excessive current flow from disrupt-
ing the operation of the circuits connected to GND. The
PGND node should be as compact and low impedance as
possible, with the negative terminals of the input and
output capacitors, the source of Q2, the LTC1430A PGND
node, the output return and the input supply return all
clustered at one point. Figure 14 is a modified schematic
showing the common connections in a proper layout. Note
that at 10A current levels or above, current density in the
PC board itself can become a concern; traces carrying high
currents should be as wide as possible.
Output Voltage Sensing
The 16-lead versions of the LTC1430A provide three pins
for sensing the output voltage: SENSE
+
, SENSE
and FB.
SENSE
+
and SENSE
connect to an internal resistor
divider which is connected to FB. To set the output of the
LTC1430A to 3.3V, connect SENSE
+
to the output as near
to the load as practical and connect SENSE
to the
common GND/PGND point. Note that SENSE
is not a true
differential input sense input; it is just the bottom of the
internal divider string. Connecting SENSE
to the ground
near the load will not improve load regulation. For any
other output voltage, the SENSE
+
and SENSE
pins should
internal 20µA source and runs at 200kHz. Connecting a
50k resistor from FREQSET to ground will sink an addi-
tional 25µA from FREQSET, causing the internal oscillator
to run at approximately 450kHz. Sourcing an external
10µA current into FREQSET will cut the internal frequency
to 100kHz. An internal clamp prevents the oscillator from
running slower than about 50kHz. Tying FREQSET to V
CC
will cause it to run at this minimum speed.
Shutdown
The LTC1430A includes a low power shutdown mode,
controlled by the logic at the SHDN pin. A high at SHDN
allows the part to operate normally. A low level at SHDN
stops all internal switching, pulls COMP and SS to ground
internally and turns Q1 and Q2 off. In shutdown, the
LTC1430A itself will drop below 1µA quiescent current
typically, although off-state leakage in the external
MOSFETs may cause the total PV
CC
current to be some-
what higher, especially at elevated temperatures. When
SHDN rises again, the LTC1430A will rerun a soft start
cycle and resume normal operation. Holding the LTC1430A
in shutdown during PV
CC
power up removes any PV
CC1
sequencing constraints.
External Clock Synchronization
The LTC1430A SHDN pin can double as an external clock
input for applications that require a synchronized clock or
a faster switching speed. The SHDN pin terminates the
internal sawtooth wave and resets the oscillator immedi-
ately when it goes low, but waits 50µs before shutting
down the rest of the internal circuitry. A clock signal
applied directly to the SHDN pin will force the LTC1430A
internal oscillator to lock to its frequency as long as the
external clock runs faster than the internal oscillator
frequency. The LTC1430A can be synchronized to fre-
quencies between 250kHz and 350kHz with no additional
components.
The LTC1430A is synchronizable at frequencies from
200kHz to 500kHz. Frequencies above 300kHz can cause
a decrease in the maximum obtainable duty cycle as rise/
fall time and propagation delay take up a large fraction of
the switch cycle. Circuits using these frequencies should
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Figure 14. Typical Schematic Showing Layout Considerations
Figure 15. Using External Resistors to Set Output Voltages
LTC1430A
V
OUT
SENSE
+
FB
R1
NC
NC
R2
SENSE
1430 F15
be floated and an external resistor string should be con-
nected to FB (Figure 15). As before, connect the top
resistor (R1) to the output as close to the load as practical
and connect the bottom resistor (R2) to the common
GND/PGND point. In both cases, connecting the top of the
resistor divider (either SENSE
+
or R1) close to the load can
significantly improve load regulation by compensating for
any drops in PC traces or hookup wires between the
LTC1430A and the load.
Power Component Hook-Up/Heat Sinking
As current levels rise much above 1A, the power compo-
nents supporting the LTC1430A start to become physi-
cally large (relative to the LTC1430A, at least) and can
require special mounting considerations. Input and output
capacitors need to carry high peak currents and must have
low ESR; this mandates that the leads be clipped as short
as possible and PC traces be kept wide and short. The
power inductor will generally be the most massive single
component on the board; it can require a mechanical hold-
down in addition to the solder on its leads, especially if it
is a surface mount type.
The power MOSFETs used require some care to ensure
proper operation and reliability. Depending on the current
levels and required efficiency, the MOSFETs chosen may
be as large as TO-220s or as small as SO-8s. High
efficiency circuits may be able to avoid heat sinking the
power devices, especially with TO-220 type MOSFETs. As
an example, a 90% efficient converter working at a steady
3.3V/10A output will dissipate only (33W/90%)10% =
3.7W. The power MOSFETs generally account for the
majority of the power lost in the converter; even assuming
that they consume 100% of the power used by the
converter, that’s only 3.7W spread over two or three
devices. A typical SO-8 MOSFET with a R
ON
suitable to
provide 90% efficiency in this design can commonly
dissipate 2W when soldered to an appropriately sized
piece of copper trace on a PC board. Slightly less efficient
or higher output current designs can often get by with
standing a TO-220 MOSFET straight up in an area with
some airflow; such an arrangement can dissipate as much
as 3W without a heat sink. Designs which must work in
high ambient temperatures or which will be routinely
overloaded will generally fare best with a heat sink.
+
+
1430 F14
3.3V
2.7µH/15A
TOTAL
1980µF
(330µF
6.3V ×6)
Q1A*
Q2*
PV
CC1
I
MAX
FREQSET
GND
PGND
SHDN
COMP
NC
SS
PV
CC2
V
CC
PGNDGND
R
C
7.5k
0.1µF
1µF
0.1µF
C
C
4700pF
C1
220pF
C
SS
0.01µF
4.7µF
35V
100
G1
I
FB
G2
FB
SENSE
+
NC
NC
LTC1430A
SENSE
GND
PGND
* MOTOROLA MTD20N03HL
MBR0530T1
5V
Q1B*
TOTAL
880µF
(220µF
10V ×4)
+
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Figure 17 is a synchronous buck regulator designed to
provide a low voltage, very high current output from a 5V
or lower input voltage. The circuit uses two 8-pin
LTC1430ACS8s, operated 180° out of phase from each
other. Each half of the circuit is good for 15A of output
current, giving 30A total. The LT
®
1006 amplifier forces the
two half circuits to share the load current equally. This
scheme trades a small amount of additional control circuit
complexity for radical reductions in the volume (hence
cost) of the capacitors and inductors required. Advan-
tages of this approach include very low input and output
ripple voltages, higher ripple frequency and extremely fast
transient response.
By incorporating two regulators phased opposite one
another, both the input ripple currents and the output
ripple currents tend to cancel. This permits running much
higher ripple currents in the output inductors than would
be tolerable with a single channel. The overall output ripple
current in a two phase design is approximately 1/2 of a
single channel’s ripple current, allowing the inductor value
of each channel to be 1/2 that of what a single channel
system would require for equal output ripple. Since energy
storage varies as the square of inductor current, and
directly as the inductance, each inductor stores only 1/8th
the energy of a single inductor design. Since there are two
inductors, total energy storage, and therefore inductor
volume, is 1/4th that of a single phase system.
A similar analysis can be done for the input capacitor
requirements. In fact, a two-phase regulator will actually
require less input capacitance than a single channel design
at 1/2 the load current. Figure 16 shows how the ripple
currents tend to cancel one another.
Another significant advantage of the two-phase topology
is radically improved transient response. During a load
transient, each of the two channels runs to maximum (or
minimum) duty cycle. The two ripple current terms now
end up reinforcing one another rather than canceling. The
result is a very high di/dt, hence, very fast transient
recoveries. Once steady state conditions return, the ripple
currents begin to cancel again, providing very low output
ripple voltage.
A + B
CHANNEL A
CHANNEL B
2µs/DIV
1430A F16
The clocking of the two channels is accomplished by the
CD4047, a low cost, CMOS mulitvibrator with a built-in
divide-by-two flip flop. The CD4047 oscillator is set to run
at 600kHz and the Q and Q outputs drive the LTC1430A
shutdown pins. Since the sync signals are derived from
the clock’s divide-by-two outputs, they are inherently
180° out of phase and at the desired 300kHz clock fre-
quency. Q1, D1 and the two resistors connected to Q1’s
base are used to disable the synchronization at turn-on to
prevent start-up problems. As long as the input-output
differential voltage is large enough to turn on Q1, the sync
circuit is disabled and both LTC1430As will free run at
200kHz. Once the output rises above 1.5V, the regula-
tors are allowed to lock to the clock.
One challenge with a voltage mode two-phase design is
current sharing. Unlike current mode control which offers
inherent current sharing, voltage mode control virtually
assures that one channel will try to hog a large percentage
of the load current. The circuit gets around this problem
with a current share amplifier. The LT1006 op amp com-
pares the voltage across both sense resistors and adds or
subtracts a small current into the lower LTC1430A’s
feedback divider, forcing it to match the upper LTC1430A’s
current. The two PCB trace resistors are intentionally
chosen to have a very low value to minimize power losses.
The LT1006 features 80µV typical V
OS
, ensuring reason-
ably accurate current sharing.
There are three problems associated with this current
sharing approach that must be dealt with. The first is that
Figure 16. Output Inductor Currents 5A/DIV, 30A Out

LTC1430AIGN#TRPBF

Mfr. #:
Manufacturer:
Analog Devices / Linear Technology
Description:
Switching Voltage Regulators Hi Pwr Buck Sw Reg Cntr
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