25
LTC1702
1702fa
The FAULT pin is an additional open-drain output that
indicates if one or both of the outputs has exceeded 15%
of its programmed output voltage. FAULT includes an
internal 10µA pull-up to V
CC
and does not require an
external pull-up to interface to standard logic. FAULT pulls
low in normal operation, and releases when a overvoltage
fault is detected.
When an overvoltage fault occurs, an internal latch sets
and FAULT goes high, disabling the LTC1702 until the
latch is cleared by recycling the power or pulling both
RUN/SS pins low simultaneously. Alternately, the FAULT
pin can be pulled back low externally with an open-
collector/open-drain device or an NFET or NPN, which will
allow the LTC1702 to resume normal operation, but will
not reset the latch. If the pull-down is later removed, the
LTC1702 will latch off again unless the latch is reset by
cycling the power or RUN/SS pins.
Note that both the PGOOD pins and the FAULT pin monitor
the output voltages by watching the FB pins. During
normal operation, each FB pin is held at a virtual ground by
the feedback amplifier, and changes at the output will not
appear at FB. This is not an issue with a properly designed
circuit, since the virtual ground at FB implies that the
output voltage is under control. If the feedback amplifier
loses control of the output, the virtual ground disappears
and the PGOOD circuit can see any output changes. This
occurs whenever the soft-start or current limit circuits are
active, whenever the MIN or MAX comparators are active,
or any time the feedback amplifier output (the COMP pin)
hits a rail or is in slew limit. Since the MAX comparator will
engage well before the output reaches the +15% fault
level, the FAULT output is largely unaffected by the virtual
ground at FB.
OPTIMIZING PERFORMANCE
2-Step Conversion
The LTC1702 is ideally suited for use in 2-step conversion
systems. 2-step systems use a primary regulator to con-
vert the input power source (batteries or AC line voltage)
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with 10mV of hysteresis, allowing fairly precise control of
the auxiliary voltage. If the LTC1702 is in discontinuous or
Burst Mode operation and the auxiliary output voltage
drops, the FCB pin will trip and the LTC1702 will resume
continuous operation regardless of the load on the main
output. The FCB pin removes the requirement that power
must be drawn from the inductor primary in order to
extract power from the auxiliary windings. With the loop in
continuous mode, the auxiliary outputs may be loaded
without regard to the primary load. Note that if the LTC1702
is already running in continuous mode and the auxiliary
output drops due to excessive loading, no additional
action can be taken by the LTC1702 to regulate the
auxiliary output.
POWER GOOD/FAULT FLAGS
The PGOOD pins report the status of the output voltage at
their respective outputs. Each is an open-drain output that
pulls low until the FB pin rises to (V
REF
– 5%), indicating
that the output voltage has risen to within 5% of the
programmed output voltage. Each PGOOD pin can inter-
face directly to standard logic inputs if an appropriate pull-
up resistor is added, or the two pins can be tied together
with a single pull-up to give a “both good” signal. Each
PGOOD pin includes an internal 100µs delay to prevent
glitches at the output from indicating false PGOOD
signals.
Figure 13. Regulating an Auxiliary Output with the FCB Pin
+
TG
LTC1702
BG
FCB
C
OUT
R
FCB1
+
C
OUT(AUX)
V
OUT(AUX)
1702 F08
+
C
IN
QT
QB
V
OUT
V
IN
R
FCB2
26
LTC1702
1702fa
to an intermediate supply voltage, often 5V. The LTC1702
then converts the intermediate voltage to the low voltage,
high current supplies required by the system. Compared
to a 1-step converter that converts a high input voltage
directly to a very low output voltage, the 2-step converter
exhibits superior transient response, smaller component
size and equivalent efficiency. Thermal management and
layout complexity are also improved with a 2-step
approach.
A typical notebook computer supply might use a 4-cell
Li-Ion battery pack as an input supply with a 15V nominal
terminal voltage. The logic circuits require 5V/3A and 3.3V/
5A to power system board logic, and 2.5V/0.5A, 1.8V/2A
and 1.5V/10A to power the CPU. A typical 2-step conver-
sion system would use a step-down switcher (perhaps an
LTC1628 or two LTC1625s) to convert 15V to 5V and
another to convert 15V to 3.3V (Figure 14). One channel of
the LTC1702 would generate the 1.5V supply using the
3.3V supply as the input and the other channel would gen-
erate 1.8V using the 5V supply as the input. The corre-
sponding 1-step system would use four similar step-down
switchers, each using 15V as the input supply and gener-
ating one of the four output voltages. Since the 2.5V sup-
ply represents a small fraction of the total output power,
either system can generate it from the 3.3V output using
an LDO linear regulator, without the 75% linear efficiency
making much of an impact on total system efficiency.
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Clearly, the 5V and 3.3V sections of the two schemes are
equivalent. The 2-step system draws additional power
from the 5V and 3.3V outputs, but the regulation tech-
niques and trade-offs at these outputs are similar. The
difference lies in the way the 1.8V and 1.5V supplies are
generated. For example, the 2-step system converts 3.3V
to 1.5V with a 45% duty cycle. During the QT on-time, the
voltage across the inductor is 1.8V and during the QB
on-time, the voltage is 1.5V, giving roughly symmetrical
transient response to positive and negative load steps. The
1.8V maximum voltage across the inductor allows the use
of a small 0.47µH inductor while keeping ripple current
under 4A (40% of the 10A maximum load). By contrast,
the 1-step converter is converting 15V to 1.5V, requiring
just a 10% duty cycle. Inductor voltages are now 13.5V
when QT is on and 1.5V when QB is on, giving vastly
different di/dt values and correspondingly skewed tran-
sient response with positive and negative current steps.
The narrow 10% duty cycle usually requires a lower
switching frequency, which in turn requires a higher value
inductor and larger output capacitor. Parasitic losses due
to the large voltage swing at the source of QT cost
efficiency, eliminating any advantage the 1-step conver-
sion might have had.
Note that power dissipation in the LTC1702 portion of a
2-step circuit is lower than it would be in a typical 1-step
converter, even in cases where the 1-step converter has
higher total efficiency than the 2-step system. In a typical
microprocessor core supply regulator, for example, the
regulator is usually located right next to the CPU. In a
1-step design, all of the power dissipated by the core
regulator is right there next to the hot CPU, aggravating
thermal management. In a 2-step LTC1702 design, a
significant percentage of the power lost in the core regu-
lation system happens in the 5V or 3.3V supply, which is
usually away from the CPU. The power lost to heat in the
LTC1702 section of the system is relatively low, minimiz-
ing the heat near the CPU.Figure 14. 2-Step Conversion Block Diagram
V
BAT
15V
LTC1628*
*OR TWO LTC1625s
LTC1702
LDO
5V/3A
1.8V/2A
1.5V/10A
3.3V/5A
2.5V/0.5A
1702 F14
27
LTC1702
1702fa
2-Step Efficiency Calculation
Calculating the efficiency of a 2-step converter system
involves some subtleties. Simply multiplying the effi-
ciency of the primary 5V or 3.3V supply by the efficiency
of the 1.8V or 1.5V supply underestimates the actual
efficiency, since a significant fraction of the total power is
drawn from the 3.3V and 5V rails in a typical system. The
correct way to calculate system efficiency is to calculate
the power lost in each stage of the converter, and divide
the total output power from all outputs by the sum of the
output power plus the power lost:
Efficiency
TotalOutputPower
TotalOutputPower TotalPowerLost
=
+
()
100%
In our example 2-step system, the total output power is:
Total output power =
15W + 16.5W + 1.25W + 3.6W + 15W = 51.35W
corresponding to 5V, 3.3V, 2.5V, 1.8V and 1.5V output
voltages.
Assuming the LTC1702 provides 90% efficiency at each
output, the additional load on the 5V and 3.3V supplies is:
1.5V: 15W/90% = 16.6W/3.3V = 5A from 3.3V
1.8V: 3.6W/90% = 4W/5V = 0.8A from 5V
2.5V: 1.25W/75% = 1.66W/3.3V = 0.5A from 3.3V
If the 5V and 3.3V supplies are each 94% efficient, the
power lost in each supply is:
1.5V: 16.6W – 15W = 1.6W
1.8V: 4W – 3.6W = 0.4W
2.5V: 1.66W – 1.25W = 0.4W
3.3V: 17.55W – 16.5W = 1W
5V: 16W – 15W = 1W
Total loss = 4.4W
Total system efficiency =
51.35W/(51.35W + 4.4W) = 92.1%
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Maximizing High Load Current Efficiency
Efficiency at high load currents (when the LTC1702 is
operating in continuous mode) is primarily controlled by
the resistance of the components in the power path
(QT, QB, L
EXT
) and power lost in the gate drive circuits due
to MOSFET gate charge. Maximizing efficiency in this
region of operation is as simple as minimizing these
terms.
The behavior of the load over time affects the efficiency
strategy. Parasitic resistances in the MOSFETs and the
inductor set the maximum output current the circuit can
supply without burning up. A typical efficiency curve
(Figure 15) shows that peak efficiency occurs near 30% of
this maximum current. If the load current will vary around
the efficiency peak and will spend relatively little time at the
maximum load, choosing components so that the average
load is at the efficiency peak is a good idea. This puts the
maximum load well beyond the efficiency peak, but usu-
ally gives the greatest system efficiency over time, which
translates to the longest run time in a battery-powered
system. If the load is expected to be relatively constant at
the maximum level, the components should be chosen so
that this load lands at the peak efficiency point, well below
the maximum possible output of the converter.
Figure 15. Typical LTC1702 Efficiency Curves
LOAD CURRENT (A)
0
70
EFFICIENCY (%)
80
90
100
510
1702 G01
15
V
IN
= 5V
V
OUT
= 3.3V
V
OUT
= 2.5V
V
OUT
= 1.6V

LTC1702IGN#PBF

Mfr. #:
Manufacturer:
Analog Devices / Linear Technology
Description:
Switching Voltage Regulators 2x 550kHz Sync 2-PhSw Reg Cntr
Lifecycle:
New from this manufacturer.
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