Two Ouput Stages Operate Antiphase Reducing
Input Capacitance and Power Supply Noise
■
5-Bit VID Control (VRM 8.4 Compliant)
V
: 1.3V to 3.5V in 50mV/100mV Steps
OUT
■
Current Mode Control Ensures Current Sharing
■
True Remote Sensing Differential Amplifier
■
OPTI-LOOPTM Compensation Minimizes C
■
Programmable Fixed Frequency: 150kHz to
OUT
300kHz—Effective 300kHz to 600kHz Switching
Frequency
■
±
1% Output Voltage Accuracy
■
Wide VIN Range: 4V to 36V Operation
■
Adjustable Soft-Start Current Ramping
■
Internal Current Foldback
■
Short-Circuit Shutdown Timer with Defeat Option
■
Overvoltage Soft-Latch Eliminates Nuisance Trips
■
Low Shutdown Current: 20µA
■
Small 36-Lead Narrow (0.209") SSOP Package
U
APPLICATIOS
■
Desktop Computers
■
Internet/Network Servers
■
Large Memory Arrays
■
DC Power Distribution Systems
■
Battery Chargers
Switching Regulator
U
DESCRIPTIO
The LTC®1709 is a 2-phase, VID programmable, synchronous step-down switching regulator controller that drives
all N-channel external power MOSFET stages in a fixed
frequency architecture. The 2-phase controller drives its
two output stages out of phase at frequencies up to
300kHz to minimize the RMS ripple currents in both input
and output capacitors. The 2-phase technique effectively
multiplies the fundamental frequency by two, improving
transient response while operating each channel at a
optimum frequency for efficiency. Thermal design is also
simplified.
An internal differential amplifier provides true remote
sensing of the regulated supply’s positive and negative
output terminals as required in high current applications.
The RUN/SS pin provides soft-start and optional timed,
short-circuit shutdown. Current foldback limits MOSFET
dissipaton during short-circuit conditions when overcurrent
latchoff is disabled. OPTI-LOOP compensation allows the
transient response to be optimized for a wide range of
output capacitors and ESR values.
, LTC and LT are registered trademarks of Linear Technology Corporation.
OPTI-LOOP is a trademark of Linear Technology Corporation.
TYPICAL APPLICATIO
S
0.1µF
V
IN
RUN/SS
1.2nF
15k
5 VID BITS
I
TH
SGND
VID0–VID4
EAIN
FBOUT
SENSEIN
V
DIFFOUT
–
V
OS
+
V
OS
Q1–Q4 2× FAIRCHILD FDS7760A OR SILICONIX Si4874
TG1
SW1
BG1
PGND
TG2
SW2
BG2
S
S
+
–
S
S
S
CC
+
–
10µF
+
LTC1709
BOOST 1
SENSE1
SENSE1
BOOST2
INTV
SENSE 2
SENSE 2
Figure 1. High Current 2-Phase Step-Down Converter
0.47µF
S
U
0.47µF
V
IN
+
5V TO 28V
V
OUT
1.3V TO 3.5V
40A
C
OUT
1000µF
4V
×2
1709 TA01
100
90
80
70
EFFICIENCY (%)
60
50
10µF ×4
Q1
Q2
Q3
Q4
35V
0.002Ω
1µH
0.002Ω
1µH
Efficiency Curve
515
10
0
LOAD CURRENTS (A)
VIN = 5V
V
f
2545
30
20
= 1.6V
OUT
= 200kHz
S
35
40
1709 TA01a
1
Page 2
LTC1709
WW
W
U
ABSOLUTE AXIU RATIGS
(Note 1)
Input Supply Voltage (VIN).........................36V to –0.3V
Topside Driver Voltages (BOOST 1, 2).......42V to –0.3V
Switch Voltage (SW1, 2) .............................36V to –5 V
SENSE 1+, SENSE 2+, SENSE 1–,
SENSE 2– Voltages....................... (1.1)INTVCC to –0.3V
EAIN, V
AMPMD, V
VID0–VID4, Voltages ...................................7V to –0.3V
Boosted Driver Voltage (BOOST-SW) ..........7V to –0.3V
PLLFLTR, PLLIN, V
ITH Voltage................................................2.7V to –0.3V
Peak Output Current <1µs(TGL1, 2; BG1, 2).............. 3A
Maximum Output CurrentOp Amp Mode; V
Maximum Output VoltageOp Amp Mode; I
= 0V1035mA
DIFFOUT
= 1mA1011V
DIFFOUT
= 1mA2MHz
DIFFOUT
SRSlew RateOp Amp Mode; RL = 2k5V/µsNote 1: Absolute Maximum Ratings are those values beyond which the
life of a device may be impaired.
Note 2: The LTC1709EG is guaranteed to meet performance specifications
from 0°C to 70°C. Specifications over the –40°C to 85°C operating
temperature range are assured by design, characterization and correlation
with statistical process controls.
Note 3: TJ is calculated from the ambient temperature TA and power
dissipation P
according to the following formulas:
D
LTC1709EG: TJ = TA + (PD • 85°C/W)Note 4: The LTC1709 is tested in a feedback loop that servos V
specified voltage and measures the resultant V
EAIN
.
ITH
to a
Note 5: Dynamic supply current is higher due to the gate charge being
Note 6: Rise and fall times are measured using 10% and 90% levels. Delay
times are measured using 50% levels.
Note 7: The minimum on-time condition corresponds to the on inductor
peak-to-peak ripple current ≥40% I
(see Minimum On-Time
MAX
Considerations in the Applications Information section).
Note 8: Each built-in pull-up resistor attached to the VID inputs also has a
series diode to allow input voltages higher than the VIDV
supply without
CC
damage or clamping (see the Applications Information section).
Note 9: When the AMPMD pin is high, the IC pins are connected directly to
the internal op amp inputs. When the AMPMD pin is low, internal MOSFET
switches connect four 40k resistors around the op amp to create a
standard unity-gain differential amp.
delivered at the switching frequency. See Applications Information.
UW
TYPICAL PERFOR A CE CHARACTERISTICS
Efficiency vs Output Current
(Figure 12)
100
80
60
40
EFFICIENCY (%)
20
0
0.1110100
VIN = 5V
VIN = 8V
VIN = 12V
VIN = 20V
V
V
f = 200kHz
OUTPUT CURRENT (A)
OUT
EXTVCC
= 2V
= 0V
1709 G01
Efficiency vs Output Current
(Figure 12)
100
V
= 2V
OUT
= 12V
V
IN
f = 200kHz
80
60
40
EFFICIENCY (%)
20
0
0.1
INTERNAL LDO VS EXTERNALLY
APPLIED 5V OVERALL EFFICIENCY
(FIGURE 12)
V
EXTVCC
V
EXTVCC
110100
OUTPUT CURRENT (A)
= 5V
= 0V
4
1709 G02
Efficiency vs Input Voltage
(Figure 12)
100
V
= 3.3V
OUT
= 5V
V
EXTVCC
= 20A
I
OUT
90
EFFICIENCY (%)
80
70
5
101520
VIN (V)
1709 G03
Page 5
UW
TEMPERATURE (°C)
–50
INTV
CC
AND EXTV
CC
SWITCH VOLTAGE (V)
4.95
5.00
5.05
2575
1709 G06
4.90
4.85
–250
50100 125
4.80
4.70
4.75
INTVCC VOLTAGE
EXTVCC SWITCHOVER THRESHOLD
TYPICAL PERFOR A CE CHARACTERISTICS
LTC1709
Supply Current vs Input Voltage
and ModeEXTVCC Voltage Drop
1000
800
600
400
SUPPLY CURRENT (µA)
200
0
05
ON
SHUTDOWN
15
10
INPUT VOLTAGE (V)
20
25
30
35
1709 G04
250
200
150
100
VOLTAGE DROP (mV)
CC
EXTV
50
0
10
0
Maximum Current Sense Threshold
Internal 5V LDO Line Reg
5.1
I
= 1mA
LOAD
5.0
4.9
4.8
VOLTAGE (V)
4.7
CC
INTV
4.6
4.5
4.4
0
510
1525
INPUT VOLTAGE (V)
203035
1709 G07
vs Duty Factor
75
50
(mV)
SENSE
V
25
0
0
20406080
30
20
CURRENT (mA)
DUTY FACTOR (%)
INTVCC and EXTVCC Switch
Voltage vs Temperature
40
50
1709 G05
Maximum Current Sense Threshold
vs Percent of Nominal Output
Voltage (Foldback)
80
70
60
50
(mV)
40
SENSE
V
30
20
10
100
1709 G08
0
0
PERCENT ON NOMINAL OUTPUT VOLTAGE (%)
25
50
75
100
1709 G09
80
60
(mV)
40
SENSE
V
20
0
Maximum Current Sense Threshold
vs V
V
SENSE(CM)
0
(Soft-Start)
RUN/SS
= 1.6V
1234
V
(V)
RUN/SS
56
1709 G10
Maximum Current Sense Threshold
vs Sense Common Mode Voltage
80
76
72
(mV)
SENSE
68
V
64
60
1
0
COMMON MODE VOLTAGE (V)
3
2
Current Sense Threshold
vs ITH Voltage
90
80
70
60
50
40
(mV)
30
20
SENSE
V
10
0
–10
–20
4
1709 G11
–30
5
0.5
0
1.5
2
1
V
(V)
ITH
2.5
1709 G12
5
Page 6
LTC1709
TEMPERATURE (°C)
–50 –25
0
EXTV
CC
SWITCH RESISTANCE (Ω)
4
10
0
50
75
1709 G22
2
8
6
25
100
125
UW
TYPICAL PERFOR A CE CHARACTERISTICS
Load RegulationV
0.0
–0.1
(%)
OUT
–0.2
NORMALIZED V
–0.3
–0.4
0
1
2
LOAD CURRENT (A)
FCB = 0V
V
= 15V
IN
FIGURE 1
3
4
5
1709 G13
Maximum Current Sense
Threshold vs Temperature
80
78
76
(mV)
SENSE
74
V
72
70
–50 –25
50
25
0
TEMPERATURE (°C)
75
100
125
1709 G17
vs V
ITH
RUN/SS
2.5
V
= 0.7V
OSENSE
2.0
1.5
(V)
ITH
V
1.0
0.5
0
0
234
1
V
RUN/SS
(V)
RUN/SS Current vs Temperature
1.8
1.6
1.4
1.2
1.0
0.8
0.6
RUN/SS CURRENT (µA)
0.4
0.2
0
–50 –25
025125
TEMPERATURE (°C)
56
7510050
1709 G14
1709 G18
SENSE Pins Total Source Current
100
50
(µA)
0
SENSE
I
–50
–100
0
24
V
COMMON MODE VOLTAGE (V)
SENSE
Soft-Start Up (Figure 12)
V
ITH
1V/DIV
V
OUT
2V/DIV
V
RUNSS
2V/DIV
100ms/DIV
6
1709 G15
1629 G19
V
OUT
50mV/DIV
I
OUT
10A/DIV
6
Load Step Response Using Active
Voltage Positioning (Figure 12)
20A
0A
20µs/DIV
1709 G20
Current Sense Pin Input Current
vs Temperature
35
EXTVCC = 5V
33
31
29
27
CURRENT SENSE INPUT CURRENT (µA)
25
–50 –25
0
TEMPERATURE (°C)
50
25
EXTVCC Switch Resistance
vs Temperature
100
125
1709 G21
75
Page 7
UW
TYPICAL PERFOR A CE CHARACTERISTICS
LTC1709
Oscillator Frequency
vs Temperature
350
300
250
200
150
FREQUENCY (kHz)
100
50
0
–50
–250
V
= 5V
FREQSET
V
= OPEN
FREQSET
V
= 0V
FREQSET
50100 125
2575
TEMPERATURE (°C)
1709 G23
Undervoltage Lockout
vs Temperature
3.50
3.45
3.40
3.35
3.30
UNDERVOLTAGE LOCKOUT (V)
3.25
3.20
–50
–250
TEMPERATURE (°C)
UUU
PI FUCTIOS
RUN/SS (Pin 1): Combination of Soft-Start, Run Control
Input and Short-Circuit Detection Timer. A capacitor to
ground at this pin sets the ramp time to full current output.
Forcing this pin below 0.8V causes the IC to shut down all
internal circuitry. All functions are disabled in shutdown.
SENSE 1+, SENSE 2+ (Pins 2,14): The (+) Input to Each
Differential Current Comparator. The ITH pin voltage and
built-in offsets between SENSE– and SENSE+ pins in
conjunction with R
SENSE 1–, SENSE 2– (Pins 3, 13): The (–) Input to the
Differential Current Comparators.
EAIN (Pin 4): Input to the Error Amplifier that compares
the feedback voltage to the internal 0.8V reference voltage.
This pin is normally connected to a resistive divider from
the output of the differential amplifier (DIFFOUT).
PLLFLTR (Pin 5): The Phase-Locked Loop’s Low Pass
Filter is tied to this pin. Alternatively, this pin can be driven
with an AC or DC voltage source to vary the frequency of
the internal oscillator.
PLLIN (Pin 6): External Synchronization Input to Phase
Detector. This pin is internally terminated to SGND with
50kΩ. The phase-locked loop will force the rising top gate
signal of controller 1 to be synchronized with the rising
edge of the PLLIN signal.
set the current trip threshold.
SENSE
V
Shutdown Latch
RUN/SS
Thresholds vs Temperature
4.5
LATCH ARMING
LATCHOFF
THRESHOLD
025125
TEMPERATURE (°C)
7510050
1709 G25
50100 125
2575
1709 G24
4.0
3.5
3.0
2.5
2.0
1.5
1.0
0.5
SHUTDOWN LATCH THRESHOLDS (V)
0
–50 –25
NC (Pins 7, 36): Do not connect.
ITH (Pin 8): Error Amplifier Output and Switching Regula-
tor Compensation Point. Both current comparator’s thresholds increase with this control voltage. The normal voltage
range of this pin is from 0V to 2.4V
SGND (Pin 9): Signal Ground, common to both controllers. Route separately to the PGND pin.
V
DIFFOUT
(Pin 10): Output of a Differential Amplifier that
provides true remote output voltage sensing. This pin
normally drives an external resistive divider that sets the
output voltage.
–
V
OS
+
, V
(Pins 11, 12): Inputs toan Operational Ampli-
OS
fier. Internal precision resistors capable of being electronically switched in or out can configure it as a differential amplifier or an uncommitted Op Amp.
ATTENOUT (Pin 15): Voltage Feedback Signal Resistively
Divided According to the VID Programming Code.
ATTENIN (Pin 16): The Input to the VID Controlled Resistive Divider.
VID0–VID4 (Pins 17,18, 19, 20, 21): VID Control Logic
Input Pins.
V
(Pin 22): Supply Pin for the VID Control Circuit.
BIAS
7
Page 8
LTC1709
PI FUCTIOS
UUU
AMPMD (Pin 23): This Logic Input pin controls the
connections of internal precision resistors that configure
the operational amplifier as a unity-gain differential
amplifier.
TG2, TG1 (Pins 24, 35): High Current Gate Drives for Top
N-Channel MOSFETS. These are the outputs of floating
drivers with a voltage swing equal to INTVCC superimposed on the switch node voltage SW.
SW2, SW1 (Pins 25, 34): Switch Node Connections to
Inductors. Voltage swing at these pins is from a Schottky
diode (external) voltage drop below ground to VIN.
BOOST 2, BOOST 1 (Pins 26, 33): Bootstrapped Supplies
to the Topside Floating Drivers. External capacitors are
connected between the Boost and Switch pins, and Schottky
diodes are connected between the Boost and INTVCC pins.
BG2, BG1 (Pins 27, 31): High Current Gate Drives for
Bottom N-Channel MOSFETS. Voltage swing at these pins
is from ground to INTVCC.
PGND (Pin 28): Driver Power Ground, connect to sources
of bottom N-channel MOSFETS and the (–) terminals of
CIN.
INTVCC (Pin 29): Output of the Internal 5V Linear Low
Dropout Regulator and the EXTVCC Switch. The driver and
control circuits are powered from this voltage source.
Decouple to power ground with a 1µF ceramic capacitor
placed directly adjacent to the IC and minimum of 4.7µF
additional tantalum or other low ESR capacitor.
EXTVCC (Pin 30): External Power Input to an Internal
Switch . This switch closes and supplies INTV
ing the internal low dropout regulator whenever EXTVCC is
higher than 4.7V. See EXTVCC Connection in the Applications Information section. Do not exceed 7V on this pin
and ensure V
VIN (Pin 32): Main Supply Pin. Should be closely decoupled
to the IC’s signal ground pin.
EXTVCC
≤ VIN.
bypass-
CC,
8
Page 9
LTC1709
UU
W
FUCTIOAL DIAGRA
PLLIN
F
IN
R
LP
C
LP
PLLFLTR
V
OS
V
OS
AMPMD
DIFFOUT
V
IN
V
IN
EXTV
INTV
5V
+
SGND
PHASE DET
50k
0.8V
+
–
CLK1
CLK2
TO
SECOND
CHANNEL
A1
–
+
V
REF
5V
LDO
REG
INTERNAL
SUPPLY
OSCILLATOR
–
+
0V POSITION
4.7V
CC
CC
DUPLICATE FOR
SECOND CHANNEL
V
IN
1.2µA
6V
4(VFB)
I1
SLOPE
COMP
SRQ
INTV
BOOST
INTV
CC
30k
30k
CC
TG
SW
BG
PGND*
SENSE
SENSE
EAIN
I
TH
RUN/SS
+
–
R
SENSE
C
C
DROP
OUT
DET
BOT
FORCE BOT
Q
SHDN
–
+–
+
45k
SHDN
RST
4(VFB)
45k
2.4V
RUN
SOFT-
START
EA
OV
SWITCH
LOGIC
–
+
+
–
TOP
BOT
INTV
V
FB
0.80V
0.86V
V
CC
IN
D
B
C
B
L
+
C
IN
C
OUT
+
V
OUT
R
C
ATTENIN
ATTENOUT
R2
20k
R1R1 VARIABLE
5-BIT VID DECODER
VID0VID1VID2VID4
VID3
TYPICAL ALL
VID PINS
40k
C
SS
V
BIAS
1709 FBD
9
Page 10
LTC1709
OPERATIO
U
(Refer to Functional Diagram)
Main Control Loop
The LTC1709 uses a constant frequency, current mode
step-down architecture with inherent current sharing.
During normal operation, the top MOSFET is turned on
each cycle when the oscillator sets the RS latch, and
turned off when the main current comparator, I1, resets
the RS latch. The peak inductor current at which I1 resets
the RS latch is controlled by the voltage on the ITH pin,
which is the output of the error amplifier EA. The differential amplifier, A1, produces a signal equal to the differential
voltage sensed across the output capacitor but re-references it to the internal signal ground (SGND) reference.
The EAIN pin receives a portion of this voltage feedback
signal at the DIFFOUT as determined by VID logic input
pins (VID0 to VID4) and is compared to the internal
reference voltage by the EA. When the load current increases, it causes a slight decrease in the EAIN pin voltage
relative to the 0.8V reference, which in turn causes the I
voltage to increase until the average inductor current
matches the new load current. After the top MOSFET has
turned off, the bottom MOSFET is turned on for the rest of
the period.
The top MOSFET drivers are biased from floating bootstrap capacitor CB, which normally is recharged during
each off cycle through an external Schottky diode. When
VIN decreases to a voltage close to V
may enter dropout and attempt to turn on the top MOSFET
continuously. A dropout detector detects this condition
and forces the top MOSFET to turn off for about 400ns
every 10th cycle to recharge the bootstrap capacitor, CB.
The main control loop is shut down by pulling Pin 1 (RUN/
SS) low. Releasing RUN/SS allows an internal 1.2µA
current source to charge soft-start capacitor CSS. When
CSS reaches 1.5V, the main control loop is enabled with the
ITH voltage clamped at approximately 30% of its maximum
value. As CSS continues to charge, ITH is gradually released allowing normal operation to resume. When the
RUN/SS pin is low, all LTC1709 functions are shut down.
If V
has charged to 4.1V, an overcurrent latchoff can be
invoked as described in the Applications Information
section.
has not reached 70% of its nominal value when C
OUT
, however, the loop
OUT
TH
SS
Low Current Operation
The LTC1709 operates in a continuous, PWM control
mode. The resulting operation at low output currents
optimizes transient response at the expense of substantial
negative inductor current during the latter part of the
period. The level of ripple current is determined by the
inductor value, input voltage, output voltage, and frequency of operation.
Frequency Synchronization
The phase-locked loop allows the internal oscillator to be
synchronized to an external source via the PLLIN pin. The
output of the phase detector at the PLLFLTR pin is also the
DC frequency control input of the oscillator that operates
over a 140kHz to 310kHz range corresponding to a DC
voltage input from 0V to 2.4V. When locked, the PLL aligns
the turn on of the top MOSFET to the rising edge of the
synchronizing signal. When PLLIN is left open, the PLLFLTR
pin goes low, forcing the oscillator to minimum frequency.
Input capacitance ESR requirements and efficiency losses
are substantially reduced because the peak current drawn
from the input capacitor is effectively divided by two and
power loss is proportional to the RMS current squared. A
two stage, single output voltage implementation can reduce input path power loss by 75% and radically reduce
the required RMS current rating of the input capacitor(s).
INTVCC/EXTVCC Power
Power for the top and bottom MOSFET drivers and most
of the IC circuitry is derived from INTVCC. When the
EXTVCC pin is left open, an internal 5V low dropout
regulator supplies INTVCC power. If the EXTVCC pin is
taken above 4.7V, the 5V regulator is turned off and an
internal switch is turned on connecting EXTVCC to INTVCC.
This allows the INTVCC power to be derived from a high
efficiency external source such as the output of the regulator itself or a secondary winding, as described in the
Applications Information section. An external Schottky
diode can be used to minimize the voltage drop from
EXTVCC to INTV
the specified INTVCC current. Voltages up to 7V can be
applied to EXTVCC for additional gate drive capability.
in applications requiring greater than
CC
10
Page 11
OPERATIO
LTC1709
U
(Refer to Functional Diagram)
Differential Amplifier
This amplifier provides true differential output voltage
sensing. Sensing both V
tion in high current applications and/or applications having electrical interconnection losses. The AMPMD pin
allows selection of internal, precision feedback resistors
for high common mode rejection differencing applications, or direct access to the actual amplifier inputs
without these internal feedback resistors for other applications. The AMPMD pin is grounded to connect the internal
precision resistors in a unity-gain differencing application,
or tied to the INTVCC pin to bypass the internal resistors
and make the amplifier inputs directly available. The
amplifier is a unity-gain stable, 2MHz gain-bandwidth,
>120dB open-loop gain design. The amplifier has an
output slew rate of 5V/µs and is capable of driving capaci-
tive loads with an output RMS current typically up to
35mA. The amplifier is not capable of sinking current and
therefore must be resistively loaded to do so.
OUT
+
and V
–
benefits regula-
OUT
Short-Circuit Detection
The RUN/SS capacitor is used initially to limit the inrush
current from the input power source. Once the controllers
have been given time, as determined by the capacitor on
the RUN/SS pin, to charge up the output capacitors and
provide full-load current, the RUN/SS capacitor is then
used as a short-circuit timeout circuit. If the output voltage
falls to less than 70% of its nominal output voltage the
RUN/SS capacitor begins discharging assuming that the
output is in a severe overcurrent and/or short-circuit
condition. If the condition lasts for a long enough period
as determined by the size of the RUN/SS capacitor, the
controller will be shut down until the RUN/SS pin voltage
is recycled. This built-in latchoff can be overidden by
providing a current >5µA at a compliance of 5V to the
RUN/SS pin. This current shortens the soft-start period
but also prevents net discharge of the RUN/SS capacitor
during a severe overcurrent and/or short-circuit condition. Foldback current limiting is activated when the output
voltage falls below 70% of its nominal level whether or not
the short-circuit latchoff circuit is enabled.
U
WUU
APPLICATIOS IFORATIO
The basic LTC1709 application circuit is shown in Figure␣ 1
on the first page. External component selection begins
with the selection of the inductor(s) based on ripple
current requirements and continues with the R
resistor selection using the calculated peak inductor current and/or maximum current limit. Next, the power
MOSFETs and D1 and D2 are selected. The operating
frequency and the inductor are chosen based mainly on
the amount of ripple current. Finally, CIN is selected for its
ability to handle the input ripple current (that PolyPhase
operation minimizes) and C
ESR to meet the output ripple voltage and load step
specifications (also minimized with PolyPhase). Current
mode architecture provides inherent current sharing between output stages. The circuit shown in Figure␣ 1 can be
configured for operation up to an input voltage of 28V
(limited by the external MOSFETs).
R
R
Selection For Output Current
SENSE
SENSE1, 2
are chosen based on the required peak output
is chosen with low enough
OUT
SENSE1, 2
TM
current. The LTC1709 current comparator has a maximum threshold of 75mV/R
mode range of SGND to 1.1( INTVCC). The current comparator threshold sets the peak inductor current, yielding
a maximum average output current I
value less half the peak-to-peak ripple current, ∆IL.
Allowing a margin for variations in the LTC1709 and
external component values yields:
R
Operating Frequency
The LTC1709 uses a constant frequency, phase-lockable
architecture with the frequency determined by an internal
capacitor. This capacitor is charged by a fixed current plus
an additional current which is proportional to the voltage
applied to the PLLFLTR pin. Refer to Phase-Locked Loop
and Frequency Synchronization in the Applications Information section for additional information.
PolyPhase is a registered trademark of Linear Technology Corporation.
SENSE
= 2(50mV/I
MAX
)
and an input common
SENSE
equal to the peak
MAX
11
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A graph for the voltage applied to the PLLFLTR pin vs
frequency is given in Figure␣ 2. As the operating frequency
is increased the gate charge losses will be higher, reducing
efficiency (see Efficiency Considerations). The maximum
switching frequency is approximately 310kHz.
2.5
2.0
1.5
1.0
PLLFLTR PIN VOLTAGE (V)
0.5
0
120170220270320
OPERATING FREQUENCY (kHz)
1709 F02
Figure 2. Operating Frequency vs V
Inductor Value Calculation and Output Ripple Current
The operating frequency and inductor selection are interrelated in that higher operating frequencies allow the use
of smaller inductor and capacitor values. So why would
anyone ever choose to operate at lower frequencies with
larger components? The answer is efficiency. A higher
frequency generally results in lower efficiency because
MOSFET gate charge and transition losses increase directly with frequency. In addition to this basic tradeoff, the
effect of inductor value on ripple current and low current
operation must also be considered. The PolyPhase approach reduces both input and output ripple currents
while optimizing individual output stages to run at a lower
fundamental frequency, enhancing efficiency.
The inductor value has a direct effect on ripple current. The
inductor ripple current ∆IL per individual section, N,
decreases with higher inductance or frequency and increases with higher VIN or V
V
∆I
OUTOUT
=−
L
fL
V
1
V
IN
:
OUT
where f is the individual output stage operating frequency.
PLLFLTR
In a 2-phase converter, the net ripple current seen by the
output capacitor is much smaller than the individual
inductor ripple currents due to ripple cancellation. The
details on how to calculate the net output ripple current
can be found in Application Note 77.
Figure 3 shows the net ripple current seen by the output
capacitors for the 1- and 2- phase configurations. The
output ripple current is plotted for a fixed output voltage as
the duty factor is varied between 10% and 90% on the
x-axis. The output ripple current is normalized against the
inductor ripple current at zero duty factor. The graph can
be used in place of tedious calculations, simplifying the
design process.
Accepting larger values of ∆IL allows the use of low
inductances, but can result in higher output voltage ripple.
A reasonable starting point for setting ripple current is ∆I
= 0.4(I
)/2, where I
OUT
is the total load current. Remem-
OUT
L
ber, the maximum ∆IL occurs at the maximum input
voltage. The individual inductor ripple currents are determined by the inductor, input and output voltages.
1.0
OUT/VIN
)]
1-PHASE
2-PHASE
)
1709 F03
0.9
0.8
0.7
0.6
/fL
0.5
O
O(P-P)
V
∆I
0.4
0.3
0.2
0.1
0
0.1 0.2 0.3 0.4
Figure 3. Normalized Output Ripple Current vs
Duty Factor [I
DUTY FACTOR (V
≈ 0.3 (∆I
RMS
0.5 0.6 0.7 0.8 0.9
O(P–P)
Inductor Core Selection
Once the values for L1 and L2 are known, the type of
inductor must be selected. High efficiency converters
generally cannot afford the core loss found in low cost
powdered iron cores, forcing the use of more expensive
ferrite, molypermalloy, or Kool Mµ® cores. Actual core
loss is independent of core size for a fixed inductor value,
Kool Mµ is a registered trademark of Magnetics, Inc.
12
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but it is very dependent on inductance selected. As inductance increases, core losses go down. Unfortunately,
increased inductance requires more turns of wire and
therefore copper losses will increase.
Ferrite designs have very low core loss and are preferred
at high switching frequencies, so design goals can concentrate on copper loss and preventing saturation. Ferrite
core material saturates “hard,” which means that inductance collapses abruptly when the peak design current is
exceeded. This results in an abrupt increase in inductor
ripple current and consequent output voltage ripple.
not allow the core to saturate!
Molypermalloy (from Magnetics, Inc.) is a very good, low
loss core material for toroids, but it is more expensive than
ferrite. A reasonable compromise from the same manufacturer is Kool Mµ. Toroids are very space efficient,
especially when you can use several layers of wire. Because they lack a bobbin, mounting is more difficult.
However, designs for surface mount are available which
do not increase the height significantly.
Power MOSFET, D1 and D2 Selection
Do
V
Main SwitchDuty Cycle
Synchronous SwitchDuty Cycle
The MOSFET power dissipations at maximum output
current are given by:
I
I
MAX
2
2
V
P
MAIN
P
SYNC
where δ is the temperature dependency of R
is a constant inversely related to the gate drive current.
OUTINMAX
=
V
2
kV
IN
()
VVVI
–
INOUTINMAX
=
OUT
=
V
IN
VV
INOUT
=
2
1
R
+
δ
()
Cf
RSS
()()
2
DS ON
2
1
+
()
()
R
δ
DS ON
+
()
–
V
IN
DS(ON)
and k
Two external power MOSFETs must be selected for each
output stage for the LTC1709: One N-channel MOSFET for
the top (main) switch, and one N-channel MOSFET for the
bottom (synchronous) switch.
The peak-to-peak drive levels are set by the INTVCC voltage. This voltage is typically 5V during start-up (see
EXTVCC Pin Connection). Consequently, logic-level threshold MOSFETs must be used in most applications. The only
exception is if low input voltage is expected (VIN < 5V);
then, sublogic-level threshold MOSFETs (V
should be used. Pay close attention to the BV
cation 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 R
input voltage, and maximum output current. When the
LTC1709 is operating in continuous mode the duty factors
for the top and bottom MOSFETs of each output stage are
given by:
, reverse transfer capacitance C
DS(ON)
GS(TH)
DSS
< 1V)
specifi-
RSS
,
Both MOSFETs have I2R losses but the topside N-channel
equation includes an additional term for transition losses,
which peak at the highest input voltage. For V
high current efficiency generally improves with larger
MOSFETs, while for V
increase to the point that the use of a higher R
with lower C
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 R
δ = 0.005/°C can be used as an approximation for low
voltage MOSFETs. C
FET characteristics. The constant k = 1.7 can be used to
estimate the contributions of the two terms in the main
switch dissipation equation.
The Schottky diodes, D1 and D2 shown in Figure 1 conduct
during the dead-time between the conduction of the two
large power MOSFETs. This helps prevent the body diode
RSS
> 20V the transition losses rapidly
IN
actual provides higher efficiency. The
vs. Temperature curve, but
DS(ON)
is usually specified in the MOS-
RSS
< 20V the
IN
DS(ON)
device
13
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of the bottom MOSFET from turning on, storing charge
during the dead-time, and requiring a reverse recovery
period which would reduce efficiency. A 1A to 3A Schottky
(depending on output current) diode 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.
CIN and C
In continuous mode, the source current of each top
N-channel MOSFET is a square wave of duty cycle V
VIN. A low ESR input capacitor sized for the maximum
RMS current must be used. The details of a closed form
equation can be found in Application Note 77. Figure 4
shows the input capacitor ripple current for a 2-phase
configuration with the output voltage fixed and input
voltage varied. The input ripple current is normalized
against the DC output current. The graph can be used in
place of tedious calculations. The minimum input ripple
current can be achieved when the input voltage is twice the
output voltage
In the graph of Figure 4, the 2-phase local maximum input
RMS capacitor currents are reached when:
V
OUT
V
IN
where k = 1, 2.
Selection
OUT
k
−21
=
4
OUT
/
These worst-case conditions are commonly used for
design because even significant deviations do not offer
much relief. Note that capacitor manufacturer’s ripple
current ratings are often based on only 2000 hours of life.
This makes it advisable to further derate the capacitor, or
to choose a capacitor rated at a higher temperature than
required. Several capacitors may also be paralleled to
meet size or height requirements in the design. Always
consult the capacitor manufacturer if there is any
question.
It is important to note that the efficiency loss is proportional to the input RMS current
squared
and therefore a
2-phase implementation results in 75% less power loss
when compared to a single phase design. Battery/input
protection fuse resistance (if used), PC board trace and
connector resistance losses are also reduced by the reduction of the input ripple current in a 2-phase system. The
required amount of input capacitance is further reduced by
the factor, 2, due to the effective increase in the frequency
of the current pulses.
The selection of C
is driven by the required effective
OUT
series resistance (ESR). Typically once the ESR requirement has been met, the RMS current rating generally far
exceeds the I
output ripple (∆V
∆∆VIESR
OUTRIPPLE
RIPPLE(P-P)
OUT
≈+
requirements. The steady state
) is determined by:
16
fC
1
OUT
0.6
0.5
0.4
0.3
0.2
DC LOAD CURRENT
RMS INPUT RIPPLE CURRNET
0.1
0
0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8
Figure 4. Normalized RMS Input Ripple Current vs
Duty Factor for 1 and 2 Output Stages
DUTY FACTOR (V
1-PHASE
2-PHASE
OUT/VIN
14
Where f = operating frequency of each stage, C
output capacitance and ∆I
RIPPLE
= combined inductor
OUT
=
ripple currents.
The output ripple varies with input voltage since ∆IL is a
function of input voltage. The output ripple will be less than
50mV at max VIN with ∆IL = 0.4I
C
C
required ESR < 4(R
OUT
> 1/(16f)(R
OUT
SENSE
SENSE
)
OUT(MAX)
) and
/2 assuming:
The emergence of very low ESR capacitors in small,
0.9
)
1709 F04
surface mount packages makes very physically small
implementations possible. The ability to externally compensate the switching regulator loop using the ITH pin(OPTILOOP compensation) allows a much wider selection of
Page 15
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output capacitor types. OPTI-LOOP compensation effectively removes constraints on output capacitor ESR. The
impedance characteristics of each capacitor type are significantly different than an ideal capacitor and therefore
require accurate modeling or bench evaluation during
design.
Manufacturers such as Nichicon, United Chemicon and
Sanyo should be considered for high performance throughhole capacitors. The OS-CON semiconductor dielectric
capacitor available from Sanyo and the Panasonic SP
surface mount types have the lowest (ESR)(size) product
of any aluminum electrolytic at a somewhat higher price.
An additional ceramic capacitor in parallel with OS-CON
type capacitors is recommended to reduce the inductance
effects.
In surface mount applications, multiple capacitors may
have to be paralleled to meet the ESR or RMS current
handling requirements of the application. Aluminum electrolytic and dry tantalum capacitors are both available in
surface mount configurations. New special polymer surface mount capacitors offer very low ESR also but have
much lower capacitive density per unit volume. In the case
of tantalum, it is critical that the capacitors are surge tested
for use in switching power supplies. Several excellent
choices are the AVX TPS, AVX TPSV or the KEMET T510
series of surface mount tantalums, available in case heights
ranging from 2mm to 4mm. Other capacitor types include
Sanyo OS-CON, Nichicon PL series and Sprague 595D
series. Consult the manufacturer for other specific recommendations. A combination of capacitors will often result
in maximizing performance and minimizing overall cost
and size.
INTVCC Regulator
An internal P-channel low dropout regulator produces 5V
at the INTVCC pin from the VIN supply pin. The INTV
regulator powers the drivers and internal circuitry of the
LTC1709. The INTVCC pin regulator can supply up to 50mA
peak and must be bypassed to power ground with a
minimum of 4.7µF tantalum or electrolytic capacitor. An
additional 1µF ceramic capacitor placed very close to the
IC is recommended due to the extremely high instantaneous currents required by the MOSFET gate drivers.
CC
High input voltage applications in which large MOSFETs
are being driven at high frequencies may cause the maximum junction temperature rating for the LTC1709 to be
exceeded. The supply current is dominated by the gate
charge supply current, in addition to the current drawn
from the differential amplifier output. The gate charge is
dependent on operating frequency as discussed in the
Efficiency Considerations section. The supply current can
either be supplied by the internal 5V regulator or via the
EXTVCC pin. When the voltage applied to the EXTVCC pin
is less than 4.7V, all of the INTVCC load current is supplied
by the internal 5V linear regulator. Power dissipation for
the IC is higher in this case by (IIN)(VIN – INTVCC) and
efficiency is lowered. The junction temperature can be
estimated by using the equations given in Note 1 of the
Electrical Characteristics. For example, the LTC1709 V
current is limited to less than 24mA from a 24V supply:
TJ = 70°C + (24mA)(24V)(85°C/W) = 119°C
Use of the EXTVCC pin reduces the junction temperature
to:
TJ = 70°C + (24mA)(5V)(85°C/W) = 80.2°C
The input supply current should be measured while the
controller is operating in continuous mode at maximum
V
and the power dissipation calculated in order to pre-
IN
vent the maximum junction temperature from being exceeded.
EXTVCC Connection
The LTC1709 contains an internal P-channel MOSFET
switch connected between the EXTVCC and INTVCC pins.
When the voltage applied to EXTV
internal regulator is turned off and an internal switch
closes, connecting the EXTV
thereby supplying internal and MOSFET gate driving power
to the IC. The switch remains closed as long as the voltage
applied to EXTVCC remains above 4.5V. This allows the
MOSFET driver and control power to be derived from the
output during normal operation (4.7V < V
from the internal regulator when the output is out of
regulation (start-up, short-circuit). Do not apply greater
than 7V to the EXTVCC pin and ensure that EXTV
0.3V when using the application circuits shown. If an
rises above 4.7V, the
CC
pin to the INTV
CC
EXTVCC
< 7V) and
CC
CC
< V
pin
IN
IN
+
15
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APPLICATIOS IFORATIO
external voltage source is applied to the EXTVCC pin when
the VIN supply is not present, a diode can be placed in
series with the LTC1709’s V
between the EXTV
and the V
CC
from backfeeding VIN.
Significant efficiency gains can be realized by powering
INTVCC from the output, since the VIN current resulting
from the driver and control currents will be scaled by the
ratio: (Duty Factor)/(Efficiency). For 5V regulators this
means connecting the EXTVCC pin directly to V
ever, for 3.3V and other lower voltage regulators, additional circuitry is required to derive INTVCC power from the
output.
The following list summarizes the four possible connections for EXTV
CC:
1. EXTVCC left open (or grounded). This will cause INTV
to be powered from the internal 5V regulator resulting in
a significant efficiency penalty at high input voltages.
2. EXTVCC connected directly to V
connection for a 5V regulator and provides the highest
efficiency.
3. EXTVCC connected to an external supply. If an external
supply is available in the 5V to 7V range, it may be used to
power EXTVCC providing it is compatible with the MOSFET
gate drive requirements.
4. EXTVCC connected to an output-derived boost network.
For 3.3V and other low voltage regulators, efficiency gains
can still be realized by connecting EXTVCC to an outputderived voltage which has been boosted to greater than
pin and a Schottky diode
IN
pin, to prevent current
IN
. How-
OUT
. This is the normal
OUT
CC
4.7V but less than 7V. This can be done with either the
inductive boost winding as shown in Figure 5a or the
capacitive charge pump shown in Figure 5b. The charge
pump has the advantage of simple magnetics.
Topside MOSFET Driver Supply (CB,DB) (Refer to
Functional Diagram)
External bootstrap capacitors CB1 and CB2 connected to
the BOOST 1 and BOOST 2 pins supply the gate drive
voltages for the topside MOSFETs. Capacitor CB in the
Functional Diagram is charged though diode DB from
INTVCC when the SW pin is low. When the topside MOSFET
turns on, the driver places the CB voltage across the gatesource of the desired MOSFET. This enhances the MOSFET
and turns on the topside switch. The switch node voltage,
SW, rises to VIN and the BOOST pin rises to VIN + V
INTVCC
.
The value of the boost capacitor CB needs to be 30 to 100
times that of the total input capacitance of the topside
MOSFET(s). The reverse breakdown of DB must be greater
than V
IN(MAX).
The final arbiter when defining the best gate drive amplitude level will be the input supply current. If a change is
made that decreases input current, the efficiency has
improved. If the input current does not change then the
efficiency has not changed either.
Output Voltage
The LTC1709 has a true remote voltage sense capablity.
The sensing connections should be returned from the load
back to the differential amplifier’s inputs through a com-
OPTIONAL EXTVCC CONNECTION
5V < V
< 7V
EXTV
SEC
LTC1709
CC
V
TG1
SW1
BG1
PGND
C
IN
IN
+
N-CH
N-CH
V
IN
1N4148
T1
R
SENSE
+
C
IN
V
IN
V
SEC
+
1µF
V
OUT
+
C
OUT
1709 F05a
EXTV
LTC1709
CC
TG1
N-CH
SW1
BG1
N-CH
PGND
V
IN
BAT850.22µF
VN2222LL
L1
Figure 5a. Secondary Output Loop with EXTVCC ConnectionFigure 5b. Capacitive Charge Pump for EXTV
16
R
SENSE
+
BAT85
BAT85
V
OUT
+
C
OUT
1709 F05b
CC
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mon, tightly coupled pair of PC traces. The differential
amplifier corrects for DC drops in both the power and
ground paths. The differential amplifier output signal is
divided down and compared with the internal precision
0.8V voltage reference by the error amplifier.
The differential amplifier can be used in either of two
configurations according to the voltage applied to the
AMPMD pin. The first configuration with the connections
illustrated in the Functional Diagram, utilizes a set of
internal, precision resistors to enable precision instrumentation-type measurement of the output voltage. This
configuration is activated when the AMPMD pin is tied to
ground. When the AMPMD pin is tied to INTVCC, the
resistors are disconnected and the amplifier inputs are
made directly available. It can be used for general uses if
the amplifier is not required for true remote sensing. The
amplifier has a 0V to 3V common mode input range
limitation due to the internal switching of its inputs. The
output uses an NPN emitter follower without any internal
pull-down current. A DC resistive load to ground is required in order to sink current. The output will swing from
0V to 10V (VIN ≥ V
DIFFOUT
Output Voltage Programming
The output voltage is digitally set to levels between 1.3V
and 3.5V using the voltage identification (VID) logic inputs
VID0 to VID4. The internal 5-bit DAC configured as a
precision resistive voltage divider sets the output voltage
in 100mV or 50mV increments according to Table 1.
The VID codes are engineered to be compatible with Intel
Pentium® II and Pentium III processor specifications for
output voltages from 1.3V to 3.5V.
The LSB (VID0) represents 50mV or 100mV increments
depending on the MSB. The MSB is VID4.
Between the ATTENOUT pin and ground is a variable
resistor, R1, whose value is controlled by the five VID input
pins (VID0 to VID4). Another resistor, R2, between the
ATTENIN and the ATTENOUT pins completes the resistive
divider. The output voltage is thus set by the ratio of
(R1␣ +␣ R2) to R1.
Pentium is a registered trademark of Intel Corporation.
+ 2V).
Table 1. VID Output Voltage Programming
VID4VID3VID2VID1VID0V
100003.50V
100013.40V
100103.30V
100113.20V
101003.10V
101013.00V
101102.90V
101112.80V
110002.70V
110012.60V
110102.50V
110112.40V
111002.30V
111012.20V
111102.10V
11111 *
000002.05V
000012.00V
000101.95V
000111.90V
001001.85V
001011.80V
001101.75V
001111.70V
010001.65V
010011.60V
010101.55V
010111.50V
011001.45V
011011.40V
011101.35V
011111.30V
* Represents codes without a defined output voltage as specified in Intel
specifications. The LTC1709 interprets these codes as a valid input and
produces an output voltage as follows: (11111) = 2V
OUT
(V)
Each VID digital input is pulled up by a 40k resistor in
series with a diode from V
. Therefore, it must be
BIAS
grounded to get a digital low input, and can be either
17
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floated or connected to V
series diode is used to prevent the digital inputs from
being damaged or clamped if they are driven higher than
V
. The digital inputs accept CMOS voltage levels.
BIAS
V
is the supply voltage for the VID section. It is
BIAS
normally connected to INTVCC but can be driven from
other sources. If it is driven from another source, that
source MUST be in the range of 2.7V to 5.5V and MUST be
alive prior to enabling the LTC1709.
Soft-Start/Run Function
The RUN/SS pin provides three functions: 1) Run/Shutdown, 2) soft-start and 3) a defeatable short-circuit latchoff
timer. Soft-start reduces the input power sources’ surge
currents by gradually increasing the controller’s current
limit I
TH(MAX)
. The latchoff timer prevents very short,
extreme load transients from tripping the overcurrent
latch. A small pull-up current (>5µA) supplied to the RUN/
SS pin will prevent the overcurrent latch from operating.
The following explanation describes how the functions
operate.
An internal 1.2µA current source charges up the soft-start
capacitor, CSS. When the voltage on RUN/SS reaches
1.5V, the controller is permitted to start operating. As the
voltage on RUN/SS increases from 1.5V to 3.0V, the
internal current limit is increased from 25mV/R
75mV/R
. The output current limit ramps up slowly,
SENSE
taking an additional 1.25s/µF to reach full current. The
output current thus ramps up slowly, reducing the starting
surge current required from the input power supply. If
RUN/SS has been pulled all the way to ground there is a
delay before starting of approximately:
15
.
t
DELAYSSSS
=
12
.
V
CsFC
A
µ
The time for the output current to ramp up is then:
315
.
VV
t
RAMPSSSS
−
=
12
.
A
µ
By pulling the RUN/SS pin below 0.8V the LTC1709 is put
into low current shutdown (IQ < 40µA). The RUN/SS pins
can be driven directly from logic as shown in Figure 6.
to get a digital high input. The
BIAS
SENSE
125
./
=µ
()
125
CsFC
./
=µ
()
to
Diode D1 in Figure 6 reduces the start delay but allows C
SS
to ramp up slowly providing the soft-start function. The
RUN/SS pin has an internal 6V zener clamp (see Functional Diagram).
D1*
INTV
CC
RSS*
RUN/SS
C
1709 F06
SS
V
3.3V OR 5VRUN/SS
*OPTIONAL TO DEFEAT OVERCURRENT LATCHOFF
IN
RSS*
D1
C
SS
Figure 6. RUN/SS Pin Interfacing
Fault Conditions: Overcurrent Latchoff
The RUN/SS pin also provides the ability to latch off the
controllers when an overcurrent condition is detected. The
RUN/SS capacitor, CSS, is used initially to limit the inrush
current of both controllers. After the controllers have been
started and been given adequate time to charge up the
output capacitors and provide full load current, the RUN/
SS capacitor is used for a short-circuit timer. If the output
voltage falls to less than 70% of its nominal value after C
SS
reaches 4.1V, CSS begins discharging on the assumption
that the output is in an overcurrent condition. If the
condition lasts for a long enough period as determined by
the size of CSS, the controller will be shut down until the
RUN/SS pin voltage is recycled. If the overload occurs
during start-up, the time can be approximated by:
t
≈ (CSS • 0.6V)/(1.2µA) = 5 • 105 (CSS)
LO1
If the overload occurs after start-up, the voltage on CSS will
continue charging and will provide additional time before
latching off:
t
≈ (CSS • 3V)/(1.2µA) = 2.5 • 106 (CSS)
LO2
This built-in overcurrent latchoff can be overridden by
providing a pull-up resistor, RSS, to the RUN/SS pin as
shown in Figure 6. This resistance shortens the soft-start
period and prevents the discharge of the RUN/SS capacitor during a severe overcurrent and/or short-circuit condition. When deriving the 5µA current from VIN as in the
figure, current latchoff is always defeated. Diode connecting this pull-up resistor to INTVCC, as in
18
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Figure␣ 6, eliminates any extra supply current during shutdown while eliminating the INTV
ing controller start-up.
Why should you defeat current latchoff? During the
prototyping stage of a design, there may be a problem with
noise pickup or poor layout causing the protection circuit
to latch off the controller. Defeating this feature allows
troubleshooting of the circuit and PC layout. The internal
short-circuit and foldback current limiting still remains
active, thereby protecting the power supply system from
failure. A decision can be made after the design is complete whether to rely solely on foldback current limiting or
to enable the latchoff feature by removing the pull-up
resistor.
The value of the soft-start capacitor CSS may need to be
scaled with output voltage, output capacitance and load
current characteristics. The minimum soft-start capacitance is given by:
CSS > (C
OUT
)(V
)(10-4)(R
OUT
The minimum recommended soft-start capacitor of CSS =
0.1µF will be sufficient for most applications.
Phase-Locked Loop and Frequency Synchronization
The LTC1709 has a phase-locked loop comprised of an
internal voltage controlled oscillator and phase detector.
This allows the top MOSFET turn-on to be locked to the
rising edge of an external source. The frequency range of
the voltage controlled oscillator is ±50% around the
center frequency fO. A voltage applied to the PLLFLTR pin
of 1.2V corresponds to a frequency of approximately
220kHz. The nominal operating frequency range of the
LTC1709 is 140kHz to 310kHz.
loading from prevent-
CC
)
SENSE
The output of the phase detector is a complementary pair
of current sources charging or discharging the external
filter network on the PLLFLTR pin. A simplified block
diagram is shown in Figure 7.
If the external frequency (f
lator frequency f
, current is sourced continuously,
0SC
) is greater than the oscil-
PLLIN
pulling up the PLLFLTR pin. When the external frequency
is less than f
, current is sunk continuously, pulling
0SC
down the PLLFLTR pin. If the external and internal frequencies are the same but exhibit a phase difference, the
current sources turn on for an amount of time corresponding to the phase difference. Thus the voltage on the
PLLFLTR pin is adjusted until the phase and frequency of
the external and internal oscillators are identical. At this
stable operating point the phase comparator output is
open and the filter capacitor CLP holds the voltage. The
LTC1709 PLLIN pin must be driven from a low impedance
source such as a logic gate located close to the pin.
The loop filter components (CLP, RLP) smooth out the
current pulses from the phase detector and provide a
stable input to the voltage controlled oscillator. The filter
components CLP and RLP determine how fast the loop
acquires lock. Typically R
=10kΩ and CLP is 0.01µF to
LP
0.1µF.
PLLIN
EXTERNAL
OSC
50k
PHASE
DETECTOR
DIGITAL
PHASE/
FREQUENCY
DETECTOR
2.4V
R
LP
10k
PLLFLTR
OSC
C
LP
The phase detector used is an edge sensitive digital type
which provides zero degrees phase shift between the
external and internal oscillators. This type of phase detector will not lock up on input frequencies close to the
harmonics of the VCO center frequency. The PLL hold-in
range, ∆fH, is equal to the capture range, ∆f
∆fH = ∆fC = ±0.5 f
O
(150kHz-300kHz)
C:
1709 F07
Figure 7. Phase-Locked Loop Block Diagram
Minimum On-Time Considerations
Minimum on-time t
ON(MIN)
is the smallest time duration
that the LTC1709 is capable of turning on the top MOSFET.
It is determined by internal timing delays and the gate
charge required to turn on the top MOSFET. Low duty cycle
19
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LTC1709
U
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APPLICATIOS IFORATIO
applications may approach this minimum on-time limit
and care should be taken to ensure that:
V
t
ON MIN
()
If the duty cycle falls below what can be accommodated by
the minimum on-time, the LTC1709 will begin to skip
cycles resulting in variable frequency operation. The output voltage will continue to be regulated, but the ripple
current and ripple voltage will increase.
The minimum on-time for the LTC1709 is generally less
than 200ns. However, as the peak sense voltage decreases, the minimum on-time gradually increases. This is
of particular concern in forced continuous applications
with low ripple current at light loads. If the duty cycle drops
below the minimum on-time limit in this situation, a
significant amount of cycle skipping can occur with correspondingly larger ripple current and voltage ripple.
If an application can operate close to the minimum ontime limit, an inductor must be chosen that has a low
enough inductance to provide sufficient ripple amplitude
to meet the minimum on-time requirement.
rule, keep the inductor ripple current of each phase equal
to or greater than 15% of I
Voltage Positioning
Voltage positioning can be used to minimize peak-to-peak
output voltage excursion under worst-case transient loading conditions. The open-loop DC gain of the control loop
is reduced depending upon the maximum load step specification. Voltage positioning can easily be added to the
LTC1709 by loading the ITH pin with a resistive divider
having a Thevenin equivalent voltage source equal to the
midpoint operating voltage of the error amplifier, or 1.2V
(see Figure 8).
The resistive load reduces the DC loop gain while maintaining the linear control range of the error amplifier. The
worst-case peak-to-peak output voltage deviation due to
transient loading can theoretically be reduced to half or
alternatively the amount of output capacitance can be
reduced for a particular application. A complete explana-
<
Vf
IN
OUT
()
OUT(MAX)
at V
As a general
IN(MAX)
.
INTV
CC
R
T2
I
TH
R
R
Figure 8. Active Voltage Positioning Applied to the LTC1709
C
T1
C
C
LTC1709
1709 F08
tion is included in Design Solutions 10 or the LTC1736
data sheet. (See www.linear-tech.com)
Efficiency Considerations
The percent efficiency of a switching regulator is equal to
the output power divided by the input power times 100%.
It is often useful to analyze individual losses to determine
what is limiting the efficiency and which change would
produce the most improvement. Percent efficiency can be
expressed as:
%Efficiency = 100% – (L1 + L2 + L3 + ...)
where L1, L2, etc. are the individual losses as a percentage
of input power.
Although all dissipative elements in the circuit produce
losses, four main sources usually account for most of the
losses in LTC1709 circuits: 1) I2R losses, 2) Topside
MOSFET transition losses, 3) INTVCC regulator current
and 4) LTC1709 VIN current (including loading on the
differential amplifier output).
1) I2R losses are predicted from the DC resistances of the
fuse (if used), MOSFET, inductor, current sense resistor,
and input and output capacitor ESR. In continuous mode
the average output current flows through L and R
SENSE
,
but is “chopped” between the topside MOSFET and the
synchronous MOSFET. If the two MOSFETs have approximately the same R
, then the resistance of one
DS(ON)
MOSFET can simply be summed with the resistances of L,
R
R
and ESR to obtain I2R losses. For example, if each
SENSE
=10mΩ, RL=10mΩ, and R
DS(ON)
=5mΩ, then the
SENSE
total resistance is 25mΩ. This results in losses ranging
from 2% to 8% as the output current increases from 3A to
15A per output stage for a 5V output, or a 3% to 12% loss
per output stage for a 3.3V output. Efficiency varies as the
inverse square of V
for the same external components
OUT
20
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LTC1709
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APPLICATIOS IFORATIO
and output power level. The combined effects of increasingly lower output voltages and higher currents required
by high performance digital systems is not doubling but
quadrupling the importance of loss terms in the switching
regulator system!
2) Transition losses apply only to the topside MOSFET(s),
and are significant only when operating at high input
voltages (typically 12V or greater). Transition losses can
be estimated from:
Transition Loss = (1.7) V
3) INTVCC current is the sum of the MOSFET driver and
control currents. The MOSFET driver current results from
switching the gate capacitance of the power MOSFETs.
Each time a MOSFET gate is switched from low to high to
low again, a packet of charge dQ moves from INTVCC to
ground. The resulting dQ/dt is a current out of INTVCC that
is typically much larger than the control circuit current. In
continuous mode, I
are the gate charges of the topside and bottom side
MOSFETs.
Supplying INTV
from an output-derived source will scale the V
required for the driver and control circuits by the ratio
(Duty Factor)/(Efficiency). For example, in a 20V to 5V
application, 10mA of INTVCC current results in approximately 3mA of VIN current. This reduces the mid-current
loss from 10% or more (if the driver was powered directly
from VIN) to only a few percent.
4) The VIN current has two components: the first is the
DC supply current given in the Electrical Characteristics
table, which excludes MOSFET driver and control currents; the second is the current drawn from the differential
amplifier output. VIN current typically results in a small
(<0.1%) loss.
Other “hidden” losses such as copper trace and internal
battery resistances can account for an additional 5% to
10% efficiency degradation in portable systems. It is very
important to include these “system” level losses in the
design of a system. The internal battery and input fuse
resistance losses can be minimized by making sure that
CIN has adequate charge storage and a very low ESR at the
switching frequency. A 50W supply will typically require a
GATECHG
power through the EXTVCC switch input
CC
2
I
IN
O(MAX) CRSS
= (QT + QB), where QT and Q
f
current
IN
B
minimum of 200µF to 300µF of output capacitance having
a maximum of 10mΩ to 20mΩ of ESR. The LTC1709
2-phase architecture typically halves the input and output
capacitance requirement over competing solutions. Other
losses including Schottky conduction losses during deadtime and inductor core losses generally account for less
than 2% total additional loss.
Checking Transient Response
The regulator loop response can be checked by looking at
the load transient response. Switching regulators take
several cycles to respond to a step in DC (resistive) load
current. When a load step occurs, V
amount equal to ∆I
series resistance of C
or discharge C
that forces the regulator to adapt to the current change and
return V
time V
ringing, which would indicate a stability problem.
OUT
OUT
OUT
to its steady-state value. During this recovery
can be monitored for excessive overshoot or
(ESR), where ESR is the effective
LOAD
• (∆I
OUT
generating the feedback error signal
) also begins to charge
LOAD
shifts by an
OUT
The
availability of the ITH pin not only allows optimization of
control loop behavior but also provides a DC coupled and
AC filtered closed loop response test point. The DC step,
rise time, and settling at this test point truly reflects the
closed loop response.
order system, phase margin and/or damping factor can be
estimated using the percentage of overshoot seen at this
pin. The bandwidth can also be estimated by examining
the rise time at the pin. The ITH external components
shown in the Figure 1 circuit will provide an adequate
starting point for most applications.
The I
loop compensation. The values can be modified slightly
(from 0.2 to 5 times their suggested values) to optimize
transient response once the final PC layout is done and the
particular output capacitor type and value have been
determined. The output capacitors need to be decided
upon because the various types and values determine the
loop gain and phase. An output current pulse of 20% to
80% of full-load current having a rise time of <2µs will
produce output voltage and ITH pin waveforms that will
give a sense of the overall loop stability without breaking
the feedback loop. The initial output voltage step resulting
from the step change in output current may not be within
series RC-CC filter sets the dominant pole-zero
TH
Assuming a predominantly second
21
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LTC1709
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APPLICATIOS IFORATIO
the bandwidth of the feedback loop, so this signal cannot
be used to determine phase margin. This is why it is better
to look at the Ith pin signal which is in the feedback loop
and is the filtered and compensated control loop response. The gain of the loop will be increased by increasing RC and the bandwidth of the loop will be increased by
decreasing CC. If RC is increased by the same factor that
CC is decreased, the zero frequency will be kept the same,
thereby keeping the phase the same in the most critical
frequency range of the feedback loop. The output voltage
settling behavior is related to the stability of the closedloop system and will demonstrate the actual overall supply
performance.
Automotive Considerations: Plugging into the
Cigarette Lighter
As battery-powered devices go mobile, there is a natural
interest in plugging into the cigarette lighter in order to
conserve or even recharge battery packs during operation.
But before you connect, be advised: you are plugging into
the supply from hell. The main battery line in an automobile is the source of a number of nasty potential transients,
including load-dump, reverse-battery, and double-battery.
Load-dump is the result of a loose battery cable. When the
cable breaks connection, the field collapse in the alternator
can cause a positive spike as high as 60V which takes
several hundred milliseconds to decay. Reverse-battery is
just what it says, while double-battery is a consequence of
tow truck operators finding that a 24V jump start cranks
cold engines faster than 12V.
The network shown in Figure 9 is the most straightforward
approach to protect a DC/DC converter from the ravages
of an automotive power line. The series diode prevents
current from flowing during reverse-battery, while the
transient suppressor clamps the input voltage during
load-dump. Note that the transient suppressor should not
conduct during double-battery operation, but must still
clamp the input voltage below breakdown of the converter.
Although the LT1709 has a maximum input voltage of 36V,
most applications will be limited to 30V by the MOSFET
BV
.
DSS
50A I
RATING
PK
12V
TRANSIENT VOLTAGE
SUPPRESSOR
GENERAL INSTRUMENT
Figure 9. Automotive Application Protection
1.5KA24A
V
IN
LTC1709
1709 F09
Design Example
As a design example, assume VIN = 5V (nominal), VIN␣ =␣ 5.5V
(max), V
= 1.8V, I
OUT
= 20A, TA = 70°C and f␣ =␣ 300kHz.
MAX
The inductance value is chosen first based on a 30% ripple
current assumption. The highest value of ripple current
occurs at the maximum input voltage. Tie the PLLFLTR pin
to the INTVCC pin for 300kHz operation. The minimum
inductance for 30% ripple current is:
≥
fI
()
≥
3003010
()()()
≥µ
135
.
−
1
∆
18
kHzA
H
V
OUTOUT
L
V
V
IN
V
.
%
1
V
18
.
55
.
V
−
A 1.5µH inductor will produce 27% ripple current. The
peak inductor current will be the maximum DC value plus
one half the ripple current, or 11.4A. The minimum ontime occurs at maximum VIN:
t
ON MIN
The R
V
OUT
==
()
SENSE
Vf
IN
5 5300
.
()()
resistors value can be calculated by using the
V
18
.
VkHz
s
=µ
11
.
maximum current sense voltage specification with some
accomodation for tolerances:
mV
R
SENSE
50
=≈Ω
11 4
0 004
.
A
.
22
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LTC1709
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APPLICATIOS IFORATIO
The power dissipation on the topside MOSFET can be
easily estimated. Using a Siliconix Si4420DY for example;
R
voltage with Tj (estimated) = 110°C at an elevated ambient
temperature:
The worst-case power disipated by the synchronous
MOSFET under normal operating conditions at elevated
ambient temperature and estimated 50°C junction temperature rise is:
A short-circuit to ground will result in a folded back current
of about:
= 0.013Ω, C
DS(ON)
P
MAIN
P
SYNC
I
=
SC
= 300pF. At maximum input
RSS
.
V
18
=
.
55
...
0 0131 7 5 510300
3000 65
()
..
5518
=
.
=
129
mV
25
0 004
.
2
1010 005 11025
()+()
V
Ω
+
kHzW
=
VV
−
.
V
55
W
1
+
Ω
2
.
[]
()()()
.
101 48 0 013
()()
2005 5
nsV
15
()
2
VApF
2
..
A
.
()
µ
.
H
CC
°− °
()
=
Ω
7
A
The duty factor for this application is:
V
DF
Using Figure 4, the RMS ripple current will be:
I
INRMS
An input capacitor(s) with a 4.6A
is required.
The output capacitor ripple current is calculated by using
the inductor ripple already calculated for each inductor
and multiplying by the factor obtained from Figure␣ 3 along
with the calculated duty factor. The output ripple in continuous mode will be highest at the maximum input
voltage since the duty factor is <50%. The maximum
output current ripple is:
∆∆I
VmAmV
O
..
V
IN
= (20A)(0.23) = 4.6A
=
COUT
I
COUTMAX
OUTRIPPLERMSRMS
V
.
18
V
5
V
OUT
fL
=
()
=
12
=Ω
201 224
.== =
036
RMS
RMS
atD F
0333
.%..
()
V
18
.
kHzH
3001 5
A
.
RMS
()
µ
.
()
.
ripple current rating
03
.
=
The worst-case power disipated by the synchronous
MOSFET under short-circuit conditions at elevated ambient temperature and estimated 50°C junction temperature
rise is:
..
5518
VV
630
−
.
55
mW
V
P
which is less than half of the normal, full-load conditions.
Incidentally, since the load no longer dissipates power in
the shorted condition, total system power dissipation is
decreased by over 99%.
SYNC
=
=
2
A
..
()
71 48 0 013
()()
Ω
PC Board Layout Checklist
When laying out the printed circuit board, the following
checklist should be used to ensure proper operation of the
LTC1709. These items are also illustrated graphically in
the layout diagram of Figure␣ 11. Check the following in
your layout:
1) Are the signal and power grounds segregated? The
LTC1709 signal ground pin should return to the (–) plate
of C
sources of the bottom N-channel MOSFETs, anodes of the
Schottky diodes, and (–) plates of CIN, which should have
as short lead lengths as possible.
2) Does the LTC1709 V
load? Does the LTC1709 V
return?
separately. The power ground returns to the
OUT
+
pin connect to the point of
OS
–
pin connect to the load
OS
23
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LTC1709
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APPLICATIOS IFORATIO
3) Are the SENSE– and SENSE+ leads routed together with
minimum PC trace spacing? The filter capacitors between
SENSE+ and SENSE– pin pairs should be as close as
possible to the LTC1709. Ensure accurate current sensing
with Kelvin connections at the current sense resistor.
4) Does the (+) plate of CIN connect to the drains of the
topside MOSFETs and the (–) plate of CIN to the sources of
the bottom MOSFETS as closely as possible? This capacitor provides the AC current to the MOSFETs. Keep the
input current path formed by the input capacitor, top and
bottom MOSFETs, and the Schottky diode on the same
side of the PC board in a tight loop to minimize conducted
and radiated EMI.
5) Is the INTVCC 1µF ceramic decoupling capacitor con-
nected closely between INTVCC and the PGND pin? This
capacitor carries the MOSFET driver peak currents. A
small value is recommended to allow placement immediately adjacent to the IC.
6) Keep the switching nodes, SW1 (SW2), away from
sensitive small-signal nodes. Ideally the switch nodes
should be placed at the furthest point from the LTC1709.
7) Use a low impedance source such as a logic gate to drive
the PLLIN pin and keep the lead as short as possible.
The diagram in Figure 10 illustrates all branch currents in
a 2-phase switching regulator. It becomes very clear after
studying the current waveforms why it is critical to keep
the high-switching-current paths to a small physical size.
High electric and magnetic fields will radiate from these
“loops” just as radio stations transmit signals. The output
capacitor ground should return to the negative terminal of
the input capacitor and not share a common ground path
with any switched current paths. The left half of the circuit
gives rise to the “noise” generated by a switching regulator. The ground terminations of the sychronous MOSFETs
and Schottky diodes should return to the negative plate(s)
of the input capacitor(s) with a short isolated PC trace
since very high switched currents are present. A separate
isolated path from the negative plate(s) of the input
capacitor(s) should be used to tie in the IC power ground
pin (PGND) and the signal ground pin (SGND). This
technique keeps inherent signals generated by high current pulses from taking alternate current paths that have
finite impedances during the total period of the switching
regulator. External OPTI-LOOP compensation allows overcompensation for PC layouts which are not optimized but
this is not the recommended design procedure.
Simplified Visual Explanation of How a 2-Phase
Controller Reduces Both Input and Output RMS Ripple
Current
A multiphase power supply significantly reduces the
amount of ripple current in both the input and output
capacitors. The effective input and output ripple frequency
is multiplied up by the number of phases used. Figure 11
graphically illustrates the principle.
The worst-case RMS ripple current for a single stage
design peaks at an input voltage of twice the output
voltage. The worst-case RMS ripple current for a two stage
design results in peak outputs of 1/4 and 3/4 of input
voltage. When the RMS current is calculated, higher
effective duty factor results and the peak current levels are
divided as long as the currents in each stage are balanced.
Refer to Application Note 77 for a detailed description of
how to calculate RMS current for the multiphase switching
regulator. Figures 3 and 4 help to illustrate how the input
and output currents are reduced by using an additional
phase. The input current peaks drop in half and the
frequency is doubled for this 2-phase converter. The input
capacity requirement is thus reduced theoretically by a
factor of four! Ceramic input capacitors with their
unbeatably low ESR characteristics can be used.
Figure 4 illustrates the RMS input current drawn from the
input capacitance vs the duty cycle as determined by the
ratio of input and output voltage. The peak input RMS
current level of the single phase system is reduced by 50%
in a 2-phase solution due to the current splitting between
the two stages.
An interesting result of the 2-phase solution is that the V
which produces worst-case ripple current for the input
capacitor, V
duces zero input current ripple in the 2-phase design.
= VIN/2, in the single phase design pro-
OUT
IN
24
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LTC1709
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APPLICATIOS IFORATIO
The output ripple current is reduced significantly when
compared to the single phase solution using the same
inductance value because the V
term from the stage that has its bottom MOSFET on
subtracts current from the (VIN - V
resulting from the stage which has its top MOSFET on. The
output ripple current is:
−−
12 1
DD
−+
12 1
∆I
RIPPLE
V
2
OUT
=
fL
where D is duty factor.
/L discharge current
OUT
)/L charging current
OUT
()
D
SW1
The input and output ripple frequency is increased by the
number of stages used, reducing the output capacity
requirements. When VIN is approximately equal to 2(V
OUT
)
as illustrated in Figures 3 and 4, very low input and output
ripple currents result.
L1
R
SENSE1
D1
V
IN
R
IN
+
C
IN
BOLD LINES INDICATE
HIGH, SWITCHING
CURRENT LINES.
KEEP LINES TO A
MINIMUM LENGTH.
SW2
L2
D2
R
SENSE2
V
OUT
C
OUT
+
R
1709 F10
L
Figure 10. Instantaneous Current Path Flow in a Multiple Phase Switching Regulator
25
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LTC1709
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APPLICATIOS IFORATIO
SW V
I
CIN
I
COUT
Figure 11. Single and 2-Phase Current Waveforms
SW1 V
SW2 V
I
CIN
I
COUT
DUAL PHASESINGLE PHASE
I
L1
I
L2
RIPPLE
1709 F11
26
Page 27
PACKAGE DESCRIPTIO
5.20 – 5.38**
(0.205 – 0.212)
LTC1709
U
Dimensions in inches (millimeters) unless otherwise noted.
G Package
36-Lead Plastic SSOP (0.209)
(LTC DWG # 05-08-1640)
12.67 – 12.93*
(0.499 – 0.509)
252622 21 20 19232427282930313233343536
7.65 – 7.90
(0.301 – 0.311)
12345678 9 10 11 1214 15 16 17 1813
1.73 – 1.99
(0.068 – 0.078)
° – 8°
0
0.13 – 0.22
(0.005 – 0.009)
NOTE: DIMENSIONS ARE IN MILLIMETERS
*
DIMENSIONS DO NOT INCLUDE MOLD FLASH. MOLD FLASH
SHALL NOT EXCEED 0.152mm (0.006") PER SIDE
**
DIMENSIONS DO NOT INCLUDE INTERLEAD FLASH. INTERLEAD
FLASH SHALL NOT EXCEED 0.254mm (0.010") PER SIDE
0.55 – 0.95
(0.022 – 0.037)
0.65
(0.0256)
BSC
0.25 – 0.38
(0.010 – 0.015)
0.05 – 0.21
(0.002 – 0.008)
G36 SSOP 1098
Information furnished by Linear Technology Corporation is believed to be accurate and reliable.
However, no responsibility is assumed for its use. Linear Technology Corporation makes no representation that the interconnection of its circuits as described herein will not infringe on existing patent rights.
27
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LTC1709
TYPICAL APPLICATIO
U
0.1µF
INTV
100pF
47k
15k
CC
3.3nF
L1
1.5µH
+
L2
1.5µH
0.004Ω
M2M1
47µF×2
35V
M4M3
0.004Ω
1000pF
10k
2.7k
51k
1000pF
470pF
SWITCHING FREQUENCY = 310kHz
MI – M4: FAIRCHILD FDS7760A
L1 – L2: SUMIDA CEP125-1R5M
1
2
3
4
5
6
7
8
9
10
11
12
13
14
15
18
RUN/SS
SENSE 1
SENSE 1
EAIN
PLLFLTR
PLLIN
NC
I
TH
SGND
V
DIFFOUT
–
V
OS
+
V
OS
SENSE 2
SENSE 2
ATTENOUT
LTC1709
+
–
–
+
TG1
SW1
BOOST 1
BG1
EXTV
INTV
PGND
BG2
BOOST 2
SW2
TG2
AMPMD
V
BIAS
VID4ATTENIN
VID3VID0
VID2VID1
36
NC
35
34
33
32
V
IN
31
30
CC
29
CC
28
27
26
25
24
23
22
2116
2017
19
VID INPUTS
C
OUTPUT CAPACITORS: PANASONIC EEFUE0G181R
OUT
D3, D4: CENTRAL CMDSH-3TR
0.22µF
1µF,25V
D4
10Ω
0.22µF
0.1µF
D3
10Ω
0.1µF
4.7µF
6.3V
+
Figure 12. 5V Input, 1.8V/20A Power Supply with Active Voltage Positioning
GND
D1
MBRM
140T3
C
D2
MBRM
140T3
OUT
+
4×180µF
4V
V
IN
5V TO 28V
V
OUT
1.3V TO 3.5V
1709 TA02
RELATED PARTS
PART NUMBERDESCRIPTIONCOMMENTS
LTC1438/LTC1439Dual High Efficiency Low Noise Synchronous Step-Down Switching Regulators POR, Auxiliary Regulator
LTC1438-ADJDual Synchronous Controller with Auxiliary RegulatorPOR, External Feedback Divider
LTC1538-AUXDual High Efficiency Low Noise Synchronous Step-Down Switching RegulatorAuxiliary Regulator, 5V Standby
LTC1539Dual High Efficiency Low Noise Synchronous Step-Down Switching Regulator5V Standby, POR, Low-Battery, Aux Regulator
LTC1436A-PLLHigh Efficiency Low Noise Synchronous Step-Down Switching RegulatorAdaptive PowerTM Mode, 24-Pin SSOP
LTC1628/LTC1628-PG Dual High Efficiency, 2-Phase Synchronous Step-Down Switching RegulatorConstant Frequency, Standby, 5V and 3.3V LDOs
LTC1629/LTC1629-PG PolyPhase High Efficiency ControllerExpandable Up to 12 Phases, G-28, Up to 120A
LTC19292-Phase High Efficiency ControllerAdjustable Output Up to 40A, G-28
LTC1702/LTC1703Dual High Efficiency, 2-Phase Synchronous Step-Down Switching Regulator500kHz, 25MHz GBW
LTC1709-7/High Efficiency, 2-Phase Synchronous Step-Down Switching Regulator with1.3V ≤ V
LTC1709-8/5-Bit VID and Power Good Indication1.1V ≤ V
LTC1709-9Current Mode Ensures Accurate Current Sharing,
3.5V ≤ V
LTC1708-PGDual High Efficiency, 2-Phase Synchronous Step-Down Switching Regulator1.3V ≤ V
with 5-Bit VID and Power Good IndicationAccurate Current Sharing, 3.5V ≤ V