Datasheet LTC3703 Datasheet (LINEAR TECHNOLOGY)

FEATURES
LOAD (A)
0
EFFICIENCY (%)
100
95
90
85
80
4
3703 F01b
1
2
3
5
VIN = 25V
VIN = 50V
VIN = 75V
High Voltage Operation: Up to 100V
Large 1Ω Gate Drivers
No Current Sense Resistor Required
Step-Up or Step-Down DC/DC Converter
Dual N-Channel MOSFET Synchronous Drive
Excellent Line and Load Transient Response
Programmable Constant Frequency: 100kHz to 600kHz
±1% Reference Accuracy
Synchronizable up to 600kHz
Selectable Pulse Skip Mode Operation
Low Shutdown Current: 50µA Typ
Programmable Current Limit
Undervoltage Lockout
Programmable Soft-Start
16-Pin Narrow SSOP and 28-Pin SSOP Packages
U
APPLICATIO S
48V Telecom and Base Station Power Supplies
Networking Equipment, Servers
Automotive and Industrial Control
, LT, LTC and LTM are registered trademarks of Linear Technology Corporation. Protected by U.S. Patents including 5408150, 5055767, 6677210, 5847554, 5481178, 6304066, 6580258.
LTC3703
100V Synchronous
Switching Regulator
Controller
U
DESCRIPTIO
®
The LTC regulator controller that can directly step-down voltages from up to 100V, making it ideal for telecom and automo­tive applications. The LTC3703 drives external N-channel MOSFETs using a constant frequency (up to 600kHz), voltage mode architecture.
A precise internal reference provides 1% DC accuracy. A high bandwidth error amplifier and patented line feed forward compensation provide very fast line and load transient response. Strong 1 gate drivers allow the LTC3703 to drive multiple MOSFETs for higher current applications. The operating frequency is user program­mable from 100kHz to 600kHz and can also be synchro­nized to an external clock for noise-sensitive applications. Current limit is programmable with an external resistor and utilizes the voltage drop across the synchronous MOSFET to eliminate the need for a current sense resistor. For applications requiring up to 60V operation with logic­level MOSFETS, refer to the LTC3703-5 data sheet.
PARAMETER LTC3703-5 LTC3703
Maximum V MOSFET Gate Drive 4.5V to 15V 9.3V to 15V VCC UV VCC UV
3703 is a synchronous step-down switching
IN
+
60V 100V
3.7V 8.7V
3.1V 6.2V
30k
10k
1000pF
100
2200pF
470pF
15k
1%
0.1µF
113k 1%
8.06k
Figure 1. High Efficiency High Voltage Step-Down Converter
MODE/SYNC
FSET
LTC3703
COMP
FB
I
MAX
INV
RUN/SS
GND
BOOST
V
DRV
BGRTN
U
9.3V TO 15V
V
IN
TG
SW
CC
CC
BG
V
CC
+
10
10µF
22µF 25V
1µF
BAS19
0.1µF
V
IN
15V TO 100V
Si7456DP
Si7456DP
MBR1100
+
8µH
68µF
270µF
16V
Efficiency vs Load Current
V
OUT
12V 5A
+
3703 F01
3703fa
1
LTC3703
1
2
3
4
5
6
7
8
9
10
11
12
13
14
TOP VIEW
G PACKAGE
28-LEAD PLASTIC SSOP
28
27
26
25
24
23
22
21
20
19
18
17
16
15
BOOST
TG
SW
NC
NC
NC
NC
V
CC
DRV
CC
BG
NC
NC
NC
BGRTN
V
IN
NC
NC
NC
NC
MODE/SYNC
f
SET
COMP
FB
I
MAX
INV
NC
RUN/SS
GND
WW
W
ABSOLUTE AXI U RATI GS
U
(Note 1)
Supply Voltages
, DRVCC.......................................... –0.3V to 15V
V
CC
(DRV
– BGRTN), (BOOST – SW) ...... –0.3V to 15V
CC
BOOST................................................ –0.3V to 115V
BGRTN ...................................................... –5V to 0V
Voltage ............................................. –0.3V to 100V
V
IN
SW Voltage ................................................ –1V to 100V
Run/SS Voltage .......................................... –0.3V to 5V
MODE/SYNC, INV Voltages....................... –0.3V to 15V
f
SET
, FB, I
Voltages ............................... – 0.3V to 3V
MAX
UUW
PACKAGE/ORDER I FOR ATIO
ORDER PART
TOP VIEW
MODE/SYNC
1
2
f
SET
3
COMP
4
FB
5
I
MAX
6
INV
7
RUN/SS
8
GND
GN PACKAGE
16-LEAD NARROW PLASTIC SSOP
T
= 150°C, θJA = 110°C/W
JMAX
V
16
IN
15
B00ST
14
TG
13
SW
12
V
CC
11
DRV
CC
10
BG
9
BGRTN
NUMBER
LTC3703EGN LTC3703IGN LTC3703HGN
GN PART
MARKING
3703 3703I 3703H
Peak Output Current <10µs BG,TG ............................ 5A
Operating Temperature Range (Note 2)
LTC3703E ............................................–40°C to 85°C
LTC3703I........................................... –40°C to 125°C
LTC3703H (Note 9) ...........................– 40°C to 150°C
Junction Temperature (Notes 3, 7)
LTC3703E, LTC3703I ....................................... 125°C
LTC3703H (Note 9) .......................................... 150°C
Storage Temperature Range ................. –65°C to 150°C
Lead Temperature (Soldering, 10 sec.)................. 300°C
ORDER PART
NUMBER
LTC3703EG
T
= 125°C, θJA = 100°C/W
JMAX
Order Options Tape and Reel: Add #TR Lead Free: Add #PBF Lead Free Tape and Reel: Add #TRPBF Lead Free Part Marking: http://www.linear.com/leadfree/
Consult LTC Marketing for parts specified with wider operating temperature ranges.
ELECTRICAL CHARACTERISTICS
temperature range, otherwise specifications are at T BGRTN = 0V, RUN/SS = I
= open, R
MAX
= 25k, unless otherwise specified.
SET
The ● denotes the specifications which apply over the full operating
= 25°C. VCC = DRVCC = V
A
= VIN = 10V, V
BOOST
MODE/SYNC
= V
INV
= VSW =
SYMBOL PARAMETER CONDITIONS MIN TYP MAX UNITS
VCC, DRV
V
IN
I
CC
CC
VCC, DRVCC Supply Voltage
V
Pin Voltage
IN
VCC Supply Current VFB = 0V
9.3 15 V
1.7 2.5 mA
RUN/SS = 0V 50 µA
I
DRVCC
I
BOOST
Main Control Loop
V
FB
2
DRVCC Supply Current (Note 5) 0 5 µA
BOOST Supply Current (Note 5), TJ 125°C
Feedback Voltage (Note 4) 0.792 0.800 0.808 V
RUN/SS = 0V 0 5 µA
> 125°C
T
J
360 500 µA 360 800 µA
RUN/SS = 0V 0 5 µA
0.788 0.812 V
100 V
3703fa
LTC3703
ELECTRICAL CHARACTERISTICS
temperature range, otherwise specifications are at T BGRTN = 0V, RUN/SS = I
= open, R
MAX
= 25k, unless otherwise specified.
SET
The ● denotes the specifications which apply over the full operating
= 25°C. VCC = DRVCC = V
A
= VIN = 10V, V
BOOST
MODE/SYNC
= V
= VSW =
INV
SYMBOL PARAMETER CONDITIONS MIN TYP MAX UNITS
V
FB, LINE
V
FB, LOAD
V
MODE/SYNC
V
MODE/SYNC
I
MODE/SYNC
V
INV
I
INV
I
VIN
I
MAX
V
OS, IMAX
V
RUN/SS
I
RUN/SS
V
UV
Feedback Voltage Line Regulation 9V < VCC < 15V (Note 4)
Feedback Voltage Load Regulation 1V < V
< 2V (Note 4)
COMP
0.007 0.05 %/V
0.01 0.1 %
MODE/SYNC Threshold MODE/SYNC Rising 0.75 0.8 0.87 V
MODE/SYNC Hysteresis 20 mV MODE/SYNC Current 0 ≤ V
MODE/SYNC
15V 0 1 µA
Invert Threshold 1 1.5 2 V Invert Current 0 ≤ V
15V 0 1 µA
INV
VIN Sense Input Current VIN = 100V 100 140 µA
I
Source Current V
MAX
V
Offset Voltage |VSW| – V
IMAX
RUN/SS = 0V, V
= 0V 10.5 12 13.5 µA
IMAX
T
IMAX
> 125°C –25 10 65 mV
J
= 10V 0 1 µA
IN
at I
= 0µA, TJ 125°C –25 10 55 mV
RUN/SS
Shutdown Threshold 0.7 0.9 1.2 V
RUN/SS Source Current RUN/SS = 0V 2.5 4 5.5 µA
Maximum RUN/SS Sink Current |VSW| – V
Undervoltage Lockout VCC Rising
V
Falling
CC
> 100mV 9 17 25 µA
IMAX
8.0 8.7 9.3 V
5.7 6.2 6.8 V
Oscillator
f
OSC
f
SYNC
t
ON, MIN
DC
MAX
Oscillator Frequency R
= 25k 270 300 330 kHz
SET
External Sync Frequency Range 100 600 kHz
Minimum On-Time 200 ns
Maximum Duty Cycle f < 200kHz 89 93 96 %
Driver
I
BG, PEAK
R
BG, SINK
I
TG, PEAK
R
TG, SINK
BG Driver Peak Source Current 1.5 2 A
BG Driver Pull-Down R
DS, ON
(Note 8) 1 1.5
TG Driver Peak Source Current 1.5 2 A
TG Driver Pull-Down R
DS, ON
(Note 8) 1 1.5
Feedback Amplifier
A
VOL
f
U
I
FB
I
COMP
Note 1: Stresses beyond those listed under Absolute Maximum Ratings may cause permanent damage to the device. Exposure to any Absolute Maximum Rating condition for extended periods may affect device reliability and lifetime.
Note 2: The LTC3703E is guaranteed to meet performance specifications from 0°C to 85°C. Specifications over the –40°C to 85°C operating temperature range are assured by design, characterization and correlation with statistical process controls. The LTC3703I is guaranteed over the full –40°C to 125°C operating junction temperature range. The LTC3703H is guaranteed over the full –40°C to 150°C operating junction temperature range.
Note 3: T
is calculated from the ambient temperature TA and power
J
dissipation PD according to the following formula:
LTC3703: T
Op Amp DC Open Loop Gain (Note 4) 74 85 dB
Op Amp Unity Gain Crossover Frequency (Note 6) 25 MHz FB Input Current 0 ≤ VFB 3V 0 1 µA
COMP Sink/Source Current ±5 ±10 mA
Note 4: The LTC3703 is tested in a feedback loop that servos V reference voltage with the COMP pin forced to a voltage between 1V and 2V.
Note 5: The dynamic input supply current is higher due to the power MOSFET gate charge being delivered at the switching frequency (Q
• f
G
OSC
Note 6: Guaranteed by design. Not subject to test. Note 7: This IC includes overtemperature protection that is intended to
protect the device during momentary overload conditions. Junction temperature will exceed 125°C when overtemperature protection is active. Continuous operation above the specified maximum operating junction temperature may impair device reliability.
guaranteed by correlation to wafer level measurement.
DS(ON)
= TA + (PD • 100 °C/W) G Package
J
Note 8: R Note 9: High junction temperatures degrade operating lifetimes. Operating
FB
).
to the
lifetime at junction temperatures greater than 125°C is derated to 1000 hours.
3703fa
3
LTC3703
UW
TYPICAL PERFOR A CE CHARACTERISTICS
TA = 25°C (unless otherwise noted).
Efficiency vs Input Voltage
100
95
90
85
EFFICIENCY (%)
80
V
= 12V
75
OUT
f = 300kHz PULSE SKIP DISABLED
70
0
10 30
V
Current vs V
CC
3.5
3.0
2.5
2.0
1.5
CURRENT (mA)
CC
V
1.0
0.5
0
6
20
810 1416
40
INPUT VOLTAGE (V)
CC
COMP = 1.5V
VCC VOLTAGE (V)
I
= 5A
OUT
50
Voltage
12
I
= 0.5A
OUT
60
VFB = 0V
70
3703 G01
3703 G04
Efficiency vs Load Current
100
95
90
85
EFFICIENCY (%)
80
75
80
70
0 0.5 1.5 2.5 3.5 4.5
Current vs Temperature
V
CC
4
3
2
CURRENT (mA)
CC
V
1
0
–50 –25 0 25
VIN = 15V
VIN = 45V
VIN = 75V
V
= 5V
OUT
f = 250kHz PULSE SKIP ENABLED
1.0 2.0 3.0 4.0 LOAD CURRENT (A)
COMP = 1.5V
VFB = 0V
50 75 125
TEMPERATURE (°C)
100
5.0
3703 G02
150
3703 G05
Load Transient Response
V
OUT
50mV/DIV
I
OUT
2A/DIV
= 50V
V
IN
= 12V
V
OUT
1A TO 5A LOAD STEP
V
Shut-Down Current vs V
CC
Voltage
100
90
80
70
60
50
40
CURRENT (µA)
CC
V
30
20
10
0
8
6
50µs/DIV
10
V
VOLTAGE (V)
CC
3703 G03
CC
12
14
16
3703 G06
V Temperature
70
65
60
55
50
CURRENT (µA)
45
CC
V
40
35
30
–50 –25 0 25
4
Shut-Down Current vs
CC
50 75 125
TEMPERATURE (°C)
100
3703 G07
0.803
0.802
0.801
0.800
REFERENCE VOLTAGE (V)
0.799
150
0.798
Reference Voltage vs Temperature
–50 –25 0 25
50 75 125
TEMPERATURE (°C)
100
3703 G08
150
Normalized Frequency vs Temperature
1.20
1.15
1.10
1.05
1.00
0.95
0.90
NORMALIZED FREQUENCY
0.85
0.80 –50 –25 0 25 50 75 100 125 150
TEMPERATURE (°C)
3703 G09
3703fa
UW
TYPICAL PERFOR A CE CHARACTERISTICS
LTC3703
Driver Peak Source Current vs Temperature
3.0 VCC = 10V
2.8
2.6
2.4
2.2
2.0
1.8
1.6
PEAK SOURCE CURRENT (A)
1.4
1.2
1.0
–50 –25 0 25
Driver Pull-Down R
50 75 125
TEMPERATURE (°C)
DS(ON)
Supply Voltage
1.1
1.0
0.9
()
DS(ON)
0.8
R
0.7
0.6
79
8
6
DRVCC/BOOST VOLTAGE (V)
11 15
10
Driver Pull-Down R
DS(ON)
vs
Temperature
1.6 VCC = 10V
1.4
1.2
1.0
()
0.8
DS(ON)
R
0.6
0.4
0.2
100
vs
150
3703 G10
0
–50 –25 0 25
50 75 125
TEMPERATURE (°C)
Rise/Fall Time vs Gate
100
150
3703 G11
Capacitance
70
DRVCC, BOOST = 10V
60
50
40
30
RISE/FALL TIME (ns)
20
10
0
0
13
14
12
3703 G13
2000 4000 8000 10000
GATE CAPACITANCE (pF)
RISE
FALL
6000
3703 G14
Driver Peak Source Current vs Supply Voltage
3.0
2.5
2.0
1.5
1.0
PEAK SOURCE CURRENT (A)
0.5
0
56 8 10 12 14
7 9 11 13
DRVCC/BOOST VOLTAGE (V)
RUN/SS Pull-Up Current vs Temperature
8
7
6
5
4
3
RUN/SS CURRENT (µA)
2
1
0
–50 –25 0 25
50 75 125
TEMPERATURE (°C)
100
15
3703 G12
150
1573 G06
RUN/SS Pull-Up Current vs V
Voltage
CC
6
5
4
3
2
RUN/SS PULLUP CURRENT (µA)
1
0
6
8101214
VCC VOLTAGE (V)
3703 G16
RUN/SS Sink Current vs SW Voltage
25
I
= 0.3V
MAX
20
15
10
5
0
RUN/SS SINK CURRENT (µA)
–5
16
–10
0
0.1 0.2
0.4 0.6 0.7
0.3 0.5
|SW| VOLTAGE (V)
3703 G17
Max % DC vs RUN/SS Voltage
100
90
80
70
60
50
40
30
MAX DUTY CYCLE (%)
20
10
0
–10
0.5
1.0 RUN VOLTAGE (V)
1.5
2.0
2.5
3.0
3703 G18
3703fa
5
LTC3703
UW
TYPICAL PERFOR A CE CHARACTERISTICS
I
Current vs Temperature
MAX
13
% Duty Cycle vs COMP Voltage
100
Max % DC vs Frequency and Temperature
100
12
SOURCE CURRENT (µA)
MAX
I
11
–50 –25 0 25 50 75 100 125 150
TEMPERATURE (°C)
Shutdown Threshold vs Temperature
1.4
1.2
1.0
0.8
0.6
0.4
SHUTDOWN THRESHOLD (V)
0.2
0
–50 –25 0 25 50 75 100 125 150 –50 –25 0 25 50 75 100 125 150
3703 G19
TEMPERATURE (°C)
VIN = 10V
80
60
VIN = 75V
40
DUTY CYCLE (%)
20
0
0.5
3703 G22 3703 G23
1.00 1.25 1.50
0.75
VIN = 25V
COMP (V)
VIN = 50V
(ns)
ON(MIN)
t
1.75 2.00
t
ON(MIN)
200
180
160
140
120
100
80
60
40
3703 G20
95
90
85
80
MAX DUTY CYCLE (%)
75
70
0 200 400 500100 300 600 700
vs Temperature
TEMPERATURE (°C)
–45°C
25°C
90°C
150°C
125°C
FREQUENCY (kHz)
3703 G21
6
3703fa
LTC3703
U
PI FU CTIO S
UU
(GN16/G28)
MODE/SYNC (Pin 1/Pin 6): Pulse Skip Mode Enable/Sync
Pin. This multifunction pin provides Pulse Skip Mode enable/disable control and an external clock input for synchronization of the internal oscillator. Pulling this pin below 0.8V or to an external logic-level synchronization signal disables Pulse Skip Mode operation and forces continuous operation. Pulling the pin above 0.8V enables Pulse Skip Mode operation. This pin can also be connected to a feedback resistor divider from a secondary winding on the inductor to regulate a second output voltage.
f
(Pin 2/Pin 7): Frequency Set. A resistor connected to
SET
this pin sets the free running frequency of the internal oscillator. See applications section for resistor value se­lection details.
COMP (Pin 3/Pin 8): Loop Compensation. This pin is connected directly to the output of the internal error ampli­fier. An RC network is used at the COMP pin to compensate the feedback loop for optimal transient response.
FB (Pin 4/Pin 9): Feedback Input. Connect FB through a resistor divider network to V
to set the output voltage.
OUT
Also connect the loop compensation network from COMP to FB.
I
(Pin 5/Pin 10): Current Limit Set. The I
MAX
MAX
pin sets the current limit comparator threshold. If the voltage drop across the bottom MOSFET exceeds the magnitude of the voltage at I I
pin has an internal 12µA current source, allowing the
MAX
, the controller goes into current limit. The
MAX
current threshold to be set with a single external resistor to ground. See the Current Limit Programming section for more information on choosing R
IMAX
.
INV (Pin 6/Pin 11): Top/Bottom Gate Invert. Pulling this pin above 2V sets the controller to operate in step-up (boost) mode with the TG output driving the synchronous MOSFET and the BG output driving the main switch. Below 1V, the controller will operate in step-down (buck) mode.
RUN/SS (Pin 7/Pin 13): Run/Soft-Start. Pulling RUN/SS below 0.9V will shut down the LTC3703, turn off both of the external MOSFET switches and reduce the quiescent supply current to 50µA. A capacitor from RUN/SS to ground will control the turn-on time and rate of rise of the output voltage at power-up. An internal 4µA current source pull-up at the RUN/SS pin sets the turn-on time at approxi­mately 750ms/µF.
GND (Pin 8/Pin 14): Ground Pin.
BGRTN (Pin 9/Pin 15): Bottom Gate Return. This pin
connects to the source of the pull-down MOSFET in the BG driver and is normally connected to ground. Connecting a negative supply to this pin allows the synchronous MOSFET’s gate to be pulled below ground to help prevent false turn-on during high dV/dt transitions on the SW node. See the Applications Information section for more details.
BG (Pin 10/Pin 19): Bottom Gate Drive. The BG pin drives the gate of the bottom N-channel synchronous switch MOSFET. This pin swings from BGRTN to DRV
DRV
(Pin 11/Pin 20): Driver Power Supply Pin. DRV
CC
CC
.
CC
provides power to the BG output driver. This pin should be connected to a voltage high enough to fully turn on the external MOSFETs, normally 10V to 15V for standard threshold MOSFETs. DRV
should be bypassed to BGRTN
CC
with a 10µF, low ESR (X5R or better) ceramic capacitor.
(Pin 12/Pin 21) : Main Supply Pin. All internal circuits
V
CC
except the output drivers are powered from this pin. V
CC
should be connected to a low noise power supply voltage between 9V and 15V and should be bypassed to GND (pin
8) with at least a 0.1µF capacitor in close proximity to the LTC3703.
SW (Pin 13/Pin 26): Switch Node Connection to Inductor and Bootstrap Capacitor. Voltage swing at this pin is from a Schottky diode (external) voltage drop below ground to V
IN
.
TG (Pin 14/Pin 27): Top Gate Drive. The TG pin drives the gate of the top N-channel synchronous switch MOSFET. The TG driver draws power from the BOOST pin and returns to the SW pin, providing true floating drive to the top MOSFET.
BOOST (Pin 15/Pin 28): Top Gate Driver Supply. The BOOST pin supplies power to the floating TG driver. The BOOST pin should be bypassed to SW with a low ESR (X5R or better) 0.1µF ceramic capacitor. An additional fast recovery Schottky diode from DRV
to BOOST will create
CC
a complete floating charge-pumped supply at BOOST.
V
(Pin 16/Pin 1): Input Voltage Sense Pin. This pin is
IN
connected to the high voltage input of the regulator and is used by the internal feedforward compensation circuitry to improve line regulation. This is not a supply pin.
3703fa
7
LTC3703
U
U
W
FU CTIO AL DIAGRA
4µA
R2
RUN/SS
C
SS
MODE/SYNC
COMP
V
R1
V
(<15V)
5
3.2V
1
3
+
0.8V
+
FB
4
16
IN
CC
12
FB
+
1V
UVSD OTSD
SYNC
DETECT
% DC
÷
LIMIT
FSET
CHIP SD
EXT SYNC
FORCED CONTINUOUS
– PWM
+
RSET
2
OSC
MIN MAX
+
0.76V
+
0.84V
OVERCURRENT
12µA
I
INV
MAX
5
R
MAX
V
CC
D
B
BOOST
15
TG
14
SW
13
DRV
CC
11
BG
10
BGRTN
9
INV
6
V
IN
C
B
M1
M2
L1
+
50mV
±
+
±
+
DRIVE LOGIC
REVERSE
CURRENT
INV
OVER
TEMP
OT SD 0.8V
V
CC
C
VCC
BANDGAP
REFERENCE
V
CC
INTERNAL
3.2V V
CC
U
OPERATIO
The LTC3703 is a constant frequency, voltage mode controller for DC/DC step-down converters. It is designed to be used in a synchronous switching architecture with two external N-channel MOSFETs. Its high operating volt­age capability allows it to directly step down input voltages up to 100V without the need for a step-down transformer. For circuit operation, please refer to the Functional Dia­gram of the IC and Figure 1. The LTC3703 uses voltage
(Refer to Functional Diagram)
OUT
V
OUT
UVLO
UV SD
GN16
GND
8
C
3703 FD
mode control in which the duty ratio is controlled directly by the error amplifier output and thus requires no current sense resistor. The V
pin receives the output voltage
FB
feedback and is compared to the internal 0.8V reference by the error amplifier, which outputs an error signal at the COMP pin. When the load current increases, it causes a drop in the feedback voltage relative to the reference. The COMP voltage then rises, increasing the duty ratio until the
3703fa
8
U
OPERATIO
output feedback voltage again matches the reference voltage. In normal operation, the top MOSFET is turned on when the RS latch is set by the on-chip oscillator and is turned off when the PWM comparator trips and resets the latch. The PWM comparator trips at the proper duty ratio by comparing the error amplifier output (after being “com­pensated” by the line feedforward multiplier) to a sawtooth waveform generated by the oscillator. When the top MOSFET is turned off, the bottom MOSFET is turned on until the next cycle begins or, if Pulse Skip Mode operation is enabled, until the inductor current reverses as deter­mined by the reverse current comparator. MAX and MIN comparators ensure that the output never exceed ±5% of nominal value by monitoring VFB and forcing the output back into regulation quickly by either keeping the top MOSFET off or forcing maximum duty cycle. The opera­tion of its other features—fast transient response, out­standing line regulation, strong gate drivers, short-circuit protection, and shutdown/soft-start—are described be­low.
Fast Transient Response
The LTC3703 uses a fast 25MHz op amp as an error amplifier. This allows the compensation network to be optimized for better load transient response. The high bandwidth of the amplifier, along with high switching frequencies and low value inductors, allow very high loop crossover frequencies. The 800mV internal reference al­lows regulated output voltages as low as 800mV without external level shifting amplifiers.
Line Feedforward Compensation
The LTC3703 achieves outstanding line transient response using a patented feedforward correction scheme. With this circuit the duty cycle is adjusted instantaneously to changes in input voltage, thereby avoiding unacceptable overshoot or undershoot. It has the added advantage of making the DC loop gain independent of input voltage. Figure 2 shows how large transient steps at the input have little effect on the output voltage.
(Refer to Functional Diagram)
LTC3703
V
OUT
50mV/DIV
V
IN
20V/DIV
I
L
2A/DIV
V
= 12V
OUT
= 1A
I
LOAD
25V TO 60V V
Figure 2. Line Transient Performance
IN
20µs/DIV
STEP
Strong Gate Drivers
The LTC3703 contains very low impedance drivers ca­pable of supplying amps of current to slew large MOSFET gates quickly. This minimizes transition losses and allows paralleling MOSFETs for higher current applications. A 100V floating high side driver drives the top side MOSFET and a low side driver drives the bottom side MOSFET (see Figure 3). They can be powered from either a separate DC supply or a voltage derived from the input or output voltage (see MOSFET Driver Supplies section). The bot­tom side driver is supplied directly from the DRV The top MOSFET drivers are biased from floating boot­strap capacitor C
, which normally is recharged during
B
each off cycle through an external diode from DRV the top MOSFET turns off. In Pulse Skip Mode operation, where it is possible that the bottom MOSFET will be off for an extended period of time, an internal counter guarantees that the bottom MOSFET is turned on at least once every 10 cycles for 10% of the period to refresh the bootstrap capacitor. An undervoltage lockout keeps the LTC3703 shut down unless this voltage is above 9V.
The bottom driver has an additional feature that helps minimize the possibility of external MOSFET shoot-thru. When the top MOSFET turns on, the switch node dV/dt pulls up the bottom MOSFET’s internal gate through the Miller capacitance, even when the bottom driver is holding the gate terminal at ground. If the gate is pulled up high enough, shoot-thru between the top side and bottom side
3703 F02
CC
CC
pin.
when
3703fa
9
LTC3703
OPERATIO
U
(Refer to Functional Diagram)
MOSFETs can occur. To prevent this from occuring, the bottom driver return is brought out as a separate pin (BGRTN) so that a negative supply can be used to reduce the effect of the Miller pull-up. For example, if a –2V supply is used on BGRTN, the switch node dV/dt could pull the gate up 2V before the V
of the bottom MOSFET has more
GS
than 0V across it.
DRV
CC
LTC3703
DRV
BGRTN
0V TO –5V
CC
BOOST
TG
SW
BG
Figure 3. Floating TG Driver Supply and Negative BG Return
V
IN
D
B
C
B
MT
MB
+
C
IN
L
3703 F03
V
OUT
+
C
OUT
Constant Frequency
The internal oscillator can be programmed with an exter­nal resistor connected from f
to ground to run between
SET
100kHz and 600kHz, thereby optimizing component size, efficiency, and noise for the specific application. The internal oscillator can also be synchronized to an external clock applied to the MODE/SYNC pin and can lock to a frequency in the 100kHz to 600kHz range. When locked to an external clock, Pulse Skip Mode operation is automati­cally disabled. Constant frequency operation brings with it a number of benefits: Inductor and capacitor values can be chosen for a precise operating frequency and the feedback loop can be similarly tightly specified. Noise generated by the circuit will always be at known frequencies. Subharmonic oscillation and slope compensation, com­mon headaches with constant frequency current mode switchers, are absent in voltage mode designs like the LTC3703.
Shutdown/Soft-Start
The main control loop is shut down by pulling RUN/SS pin low. Releasing RUN/SS allows an internal 4µA current source to charge the soft-start capacitor C
. When C
SS
SS
reaches 1V, the main control loop is enabled with the duty
cycle control set to 0%. As C
continues to charge, the
SS
duty cycle is gradually increased, allowing the output voltage to rise. This soft-start scheme smoothly ramps the output voltage to its regulated value, with no overshoot. The RUN/SS voltage will continue ramping until it reaches an internal 4V clamp. Then the MIN feedback comparator is enabled and the LTC3703 is in full operation. When the RUN/SS is low, the supply current is reduced to 50µA.
V
OUT
V
RUN/SS
1.4V
0V
4V
3V
1V
0V
SHUTDOWN
LTC3703
ENABLE
START-UP
MINIMUM
DUTY CYCLE
POWER
DOWN MODE
NORMAL OPERATION
MIN COMPARATOR ENABLED
OUTPUT VOLTAGE IN REGULATION
RUN/SS SOFT-STARTS OUTPUT VOLTAGE AND INDUCTOR CURRENT
CURRENT
LIMIT
3703 F04
Figure 4. Soft-Start Operation in Start Up and Current Limit
Current Limit
The LTC3703 includes an onboard current limit circuit that limits the maximum output current to a user-programmed level. It works by sensing the voltage drop across the bottom MOSFET and comparing that voltage to a user­programmed voltage at the I
pin. Since the bottom
MAX
MOSFET looks like a low value resistor during its on-time, the voltage drop across it is proportional to the current flowing in it. In a buck converter, the average current in the inductor is equal to the output current. This current also flows through the bottom MOSFET during its on-time. Thus by watching the drain-to-source voltage when the bottom MOSFET is on, the LTC3703 can monitor the output current. The LTC3703 senses this voltage and inverts it to allow it to compare the sensed voltage (which becomes more negative as peak current increases) with a positive voltage at the I 12µA pull-up, enabling the user to set the voltage at I with a single resistor (R Limit Programming section for R
pin. The I
MAX
) to ground. See the Current
IMAX
IMAX
pin includes a
MAX
selection.
MAX
3703fa
10
OPERATIO
LTC3703
U
For maximum protection, the LTC3703 current limit con­sists of a steady-state limit circuit and an instantaneous limit circuit. The steady-state limit circuit is a g
amplifier
m
that pulls a current from the RUN/SS pin proportional to the difference between the SW and I
voltages. This
MAX
current begins to discharge the capacitor at RUN/SS, reducing the duty cycle and controlling the output voltage until the current regulates at the limit. Depending on the size of the capacitor, it may take many cycles to discharge the RUN/SS voltage enough to properly regulate the output current. This is where the instantaneous limit circuit comes into play. The instantaneous limit circuit is a cycle-by-cycle comparator which monitors the bottom MOSFET’s drain voltage and keeps the top MOSFET from turning on whenever the drain voltage is 50mV above the programmed max drain voltage. Thus the cycle-by-cycle comparator will keep the inductor current under control until the g
amplifier gains control.
m
Pulse Skip Mode
The LTC3703 can operate in one of two modes selectable with the MODE/SYNC pin—Pulse Skip Mode or forced continuous mode. Pulse Skip Mode is selected when increased efficiency at light loads is desired. In this mode, the bottom MOSFET is turned off when inductor current reverses to minimize the efficiency loss due to reverse current flow. As the load is decreased (see Figure 6), the duty cycle is reduced to maintain regulation until its minimum on-time (~200ns) is reached. When the load decreases below this point, the LTC3703 begins to skip
cycles to maintain regulation. The frequency drops but this further improves efficiency by minimizing gate charge losses. In forced continuous mode, the bottom MOSFET is always on when the top MOSFET is off, allowing the inductor current to reverse at low currents. This mode is less efficient due to resistive losses, but has the advantage of better transient response at low currents, constant frequency operation, and the ability to maintain regulation when sinking current. See Figure 5 for a comparison of the effect on efficiency at light loads for each mode. The MODE/SYNC threshold is 0.8V ±7.5%, allowing the MODE/ SYNC to act as a feedback pin for regulating a second winding. If the feedback voltage drops below 0.8V, the LTC3703 reverts to continuous operation to maintain regulation in the secondary supply.
100
VIN = 25V
90
VIN = 75V
80
70
60
50
40
EFFICIENCY (%)
30
20
10
0
10
Figure 5. Efficiency in Pulse Skip/Forced Continuous Modes
VIN = 25V
VIN = 75V
FORCED CONTINUOUS PULSE SKIP MODE
100 1000 10000
LOAD (mA)
3703 F05
PULSE SKIP MODE
DECREASING
LOAD
CURRENT
Figure 6. Comparison of Inductor Current Waveforms for Pulse Skip Mode and Forced Continuous Operation
FORCED CONTINUOUS
3703 F06
3703fa
11
LTC3703
Rk
f kHz
SET
()
()
=
7100
25
U
OPERATIO
Buck or Boost Mode Operation
The LTC3703 has the capability of operating both as a step-down (buck) and step-up (boost) controller. In boost mode, output voltages as high as 80V can be tightly regulated. With the INV pin grounded, the LTC3703 oper­ates in buck mode with TG driving the main (top side) switch and BG driving the synchronous (bottom side) switch. If the INV pin is pulled above 2V, the LTC3703 operates in boost mode with BG driving the main (bottom side) switch and TG driving the synchronous (top side) switch. Internal circuit operation is very similar regardless
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APPLICATIO S I FOR ATIO
The basic LTC3703 application circuit is shown in Figure 1. External component selection is determined by the input voltage and load requirements as explained in the following sections. After the operating frequency is se­lected, R and the inductor are chosen for a desired amount of ripple current and also to optimize efficiency and component size. Next, the power MOSFETs and D1 are selected based on voltage, load and efficiency requirements. C lected for its ability to handle the large RMS currents in the converter and C meet the output voltage ripple and transient specifica­tions. Finally, the loop compensation components are chosen to meet the desired transient specifications.
and L can be chosen. The operating frequency
SET
is se-
IN
is chosen with low enough ESR to
OUT
of the operating mode with the following exceptions: In boost mode, Pulse Skip Mode operation is always dis­abled regardless of the level of the MODE/SYNC pin and the line feedforward compensation is also disabled. The overcurrent circuitry continues to monitor the load current by looking at the drain voltage of the main (bottom side) MOSFET. In boost mode, however, the peak MOSFET current does not equal the load current but instead I
= I
D
account when programming the I
noise-
/(1 – D). This factor needs to be taken into
LOAD
voltage.
MAX
sensitive communications systems, it is often de­sirable to keep the switching noise out of a sensitive frequency band.
The LTC3703 uses a constant frequency architecture that can be programmed over a 100kHz to 600kHz range with a single resistor from the f Figure 1. The nominal voltage on the f
pin to ground, as shown in
SET
pin is 1.2V, and
SET
the current that flows from this pin is used to charge and discharge an internal oscillator capacitor. The value of R
for a given operating frequency can be chosen from
SET
Figure 7 or from the following equation:
Operating Frequency
The choice of operating frequency and inductor value is a trade off between efficiency and component size. Low frequency operation improves efficiency by reducing MOSFET switching losses and gate charge losses. How­ever, lower frequency operation requires more induc­tance for a given amount of ripple current, resulting in a larger inductor size and higher cost. If the ripple current is allowed to increase, larger output capacitors may be required to maintain the same output ripple. For convert­ers with high step-down VIN to V
ratios, another
OUT
consideration is the minimum on-time of the LTC3703 (see the Minimum On-time Considerations section). A final consideration for operating frequency is that in
12
1000
100
(k)
SET
R
10
1
200 1000800600400
0
Figure 7. Timing Resistor (R
FREQUENCY (kHz)
SET
3703 F07
) Value
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APPLICATIO S I FOR ATIO
LTC3703
The oscillator can also be synchronized to an external clock applied to the MODE/SYNC pin with a frequency in the range of 100kHz to 600kHz (refer to the MODE/SYNC Pin section for more details). In this synchronized mode, Pulse Skip Mode operation is disabled. The clock high level must exceed 2V for at least 25ns. As shown in Figure 8, the top MOSFET turn-on will follow the rising edge of the external clock by a constant delay equal to one­tenth of the cycle period.
MODE/
SYNC
TG
I
L
Figure 8. MODE/SYNC Clock Input and Switching Waveforms for Synchronous Operation
t
MIN
= 25ns
0.8T
D = 40%
T T = 1/f
2V TO 10V
O
0.1T
3703 F08
Inductor
The inductor in a typical LTC3703 circuit is chosen for a specific ripple current and saturation current. Given an input voltage range and an output voltage, the inductor value and operating frequency directly determine the ripple current. The inductor ripple current in the buck mode is:
I
=
L
V
OUT OUT
fL
()()
1
⎜ ⎝
V
⎟ ⎠
V
IN
Lower ripple current reduces core losses in the inductor, ESR losses in the output capacitors and output voltage ripple. Thus highest efficiency operation is obtained at low frequency with small ripple current. To achieve this how­ever, requires a large inductor.
A reasonable starting point is to choose a ripple current between 20% and 40% of I
. Note that the largest
O(MAX)
ripple current occurs at the highest V
. To guarantee that
IN
ripple current does not exceed a specified maximum, the inductor in buck mode should be chosen according to:
L
V
OUT
fI
LMAX
1
V
() ()
V
IN MAX
OUT
⎞ ⎟
The inductor also has an affect on low current operation when Pulse Skip Mode operation is enabled. The fre­quency begins to decrease when the output current drops below the average inductor current at which the LTC3703 is operating at its t
ON(MIN)
in discontinuous mode (see Figure 6). Lower inductance increases the peak inductor current that occurs in each minimum on-time pulse and thus increases the output current at which the frequency starts decreasing.
Power MOSFET Selection
The LTC3703 requires at least two external N-channel power MOSFETs, one for the top (main) switch and one or more for the bottom (synchronous) switch. The number, type and “on” resistance of all MOSFETs selected take into account the voltage step-down ratio as well as the actual position (main or synchronous) in which the MOSFET will be used. A much smaller and much lower input capaci­tance MOSFET should be used for the top MOSFET in applications that have an output voltage that is less than 1/3 of the input voltage. In applications where V
IN
>> V
OUT
, the top MOSFETs’ “on” resistance is normally less impor­tant for overall efficiency than its input capacitance at operating frequencies above 300kHz. MOSFET manufac­turers have designed special purpose devices that provide reasonably low “on” resistance with significantly reduced input capacitance for the main switch application in switch­ing regulators.
Selection criteria for the power MOSFETs include the “on” resistance R
, input capacitance, breakdown voltage
DS(ON)
and maximum output current.
The most important parameter in high voltage applica­tions is breakdown voltage BV
. Both the top and
DSS
bottom MOSFETs will see full input voltage plus any additional ringing on the switch node across its drain-to­source during its off-time and must be chosen with the
3703fa
13
LTC3703
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APPLICATIO S I FOR ATIO
appropriate breakdown specification. Since many high voltage MOSFETs have higher threshold voltages (typi­cally, V
GS(MIN)
with a 9V to 15V gate drive supply (DRV
For maximum efficiency, on-resistance R capacitance should be minimized. Low R
≥ 6V), the LTC3703 is designed to be used
pin).
CC
and input
DS(ON)
minimizes
DS(ON)
conduction losses and low input capacitance minimizes transition losses. MOSFET input capacitance is a combi­nation of several components but can be taken from the typical “gate charge” curve included on most data sheets (Figure 9).
V
IN
V
GS
MILLER EFFECT
ab
Q
C
MILLER
IN
= (QB – QA)/V
Figure 9. Gate Charge Characteristic
DS
V
+
V
+
V
GS
DS
3703 F09
The curve is generated by forcing a constant input current into the gate of a common source, current source loaded stage and then plotting the gate voltage versus time. The initial slope is the effect of the gate-to-source and the gate­to-drain capacitance. The flat portion of the curve is the result of the Miller multiplication effect of the drain-to-gate capacitance as the drain drops the voltage across the current source load. The upper sloping line is due to the drain-to-gate accumulation capacitance and the gate-to­source capacitance. The Miller charge (the increase in coulombs on the horizontal axis from a to b while the curve is flat) is specified for a given V adjusted for different V
voltages by multiplying by the
DS
ratio of the application V values. A way to estimate the C
drain voltage, but can be
DS
to the curve specified V
DS
term is to take the
MILLER
DS
change in gate charge from points a and b on a manufac­turers data sheet and divide by the stated V specified. C
is the most important selection criteria
MILLER
voltage
DS
for determining the transition loss term in the top MOSFET but is not directly specified on MOSFET data sheets. C
RSS
and COS are specified sometimes but definitions of these parameters are not included.
When the controller is operating in continuous mode the duty cycles for the top and bottom MOSFETs are given by:
V
MainSwitchDutyCycle
SynchronousSwitchDutyCycle
OUT
=
V
IN
VV
IN OUT
=
V
IN
The power dissipation for the main and synchronous MOSFETs at maximum output current are given by:
V
P
MAIN
OUT
=
()
V
IN
I
2
MAX
V
IN
⎡ ⎢
VV V
CC TH IL TH IL
VV
IN OUT
SYNC
=
V
IN
P
where δ is the temperature dependency of R
2
IR
MAX DS ON
11
++
12()
δ
()
(
RRC
)( ) •
DR MILLER
+
() ()
()()
IR
MAX DS N20
+
1 δ
⎥ ⎥⎥
()
f
()
DS(ON)
, RDR is
the effective top driver resistance (approximately 2 at V
= V
GS
in drain potential in the particular application. V
), VIN is the drain potential
MILLER
and
the change
TH(IL)
is the data sheet specified typical gate threshold voltage speci­fied in the power MOSFET data sheet at the specified drain current. C
is the calculated capacitance using the
MILLER
gate charge curve from the MOSFET data sheet and the technique described above.
Both MOSFETs have I2R losses while the topside N-channel equation includes an additional term for transition losses, which peak at the highest input voltage. For V
< 25V, the
IN
high current efficiency generally improves with larger MOSFETs, while for V
> 25V, the transition losses
IN
rapidly increase to the point that the use of a higher R
device with lower C
DS(ON)
actually provides higher
MILLER
efficiency. The 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
vs temperature curve, and
DS(ON)
typically varies from 0.005/°C to 0.01/°C depending on the particular MOSFET used.
3703fa
14
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APPLICATIO S I FOR ATIO
LTC3703
Multiple MOSFETs can be used in parallel to lower R
DS(ON)
and meet the current and thermal requirements if desired. The LTC3703 contains large low impedance drivers ca­pable of driving large gate capacitances without signifi­cantly slowing transition times. In fact, when driving MOSFETs with very low gate charge, it is sometimes helpful to slow down the drivers by adding small gate resistors (5 or less) to reduce noise and EMI caused by the fast transitions.
Schottky Diode Selection
The Schottky diode D1 shown in Figure 1 conducts during the dead time between the conduction of the power MOSFETs. This prevents the body diode of the bottom MOSFET from turning on and storing charge during the dead time and requiring a reverse recovery period that could cost as much as 1% to 2% in efficiency. A 1A Schottky diode is generally a good size for 3A to 5A regulators. Larger diodes result in additional losses due to their larger junction capacitance. The diode can be omitted if the efficiency loss can be tolerated.
Input Capacitor Selection
In continuous mode, the drain current of the top MOSFET is approximately a square wave of duty cycle V
OUT/VIN
which must be supplied by the input capacitor. To prevent large input transients, a low ESR input capacitor sized for the maximum RMS current is given by:
Because tantalum and OS-CON capacitors are not avail­able in voltages above 30V, for regulators with input supplies above 30V, choice of input capacitor type is limited to ceramics or aluminum electrolytics. Ceramic capacitors have the advantage of very low ESR and can handle high RMS current, however ceramics with high voltage ratings (>50V) are not available with more than a few microfarads of capacitance. Furthermore, ceramics have high voltage coefficients which means that the ca­pacitance values decrease even more when used at the rated voltage. X5R and X7R type ceramics are recom­mended for their lower voltage and temperature coeffi­cients. Another consideration when using ceramics is their high Q which if not properly damped, may result in excessive voltage stress on the power MOSFETs. Alumi­num electrolytics have much higher bulk capacitance, however, they have higher ESR and lower RMS current ratings.
A good approach is to use a combination of aluminum electrolytics for bulk capacitance and ceramics for low ESR and RMS current. If the RMS current cannot be handled by the aluminum capacitors alone, when used together, the percentage of RMS current that will be supplied by the aluminum capacitor is reduced to approxi­mately:
%
I
RMS ALUM
,
()
fCR
+118
ESR
•%
100
2
/
IN
1
⎟ ⎠
= 2V
12
OUT
, where I
RMS
V
II
() ()
CIN RMS O MAX
OUTININ
V
V
⎜ ⎝
V
OUT
This formula has a maximum at V = I
/2. This simple worst-case condition is com-
O(MAX)
monly used for design because even significant deviations do not offer much relief. Note that the ripple current ratings from capacitor manufacturers 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 placed in parallel to meet size or height requirements in the design.
where R
is the ESR of the aluminum capacitor and C is
ESR
the overall capacitance of the ceramic capacitors. Using an aluminum electrolytic with a ceramic also helps damp the high Q of the ceramic, minimizing ringing.
Output Capacitor Selection
The selection of C
is primarily determined by the ESR
OUT
required to minimize voltage ripple. The output ripple (V
) is approximately equal to:
OUT
V I ESR
∆≤+
OUT L
⎛ ⎜
8
fC
1
OUT
⎞ ⎟
3703fa
15
LTC3703
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APPLICATIO S I FOR ATIO
Since ∆IL increases with input voltage, the output ripple is highest at maximum input voltage. ESR also has a signifi­cant effect on the load transient response. Fast load transitions at the output will appear as voltage across the ESR of C
until the feedback loop in the LTC3703 can
OUT
change the inductor current to match the new load current value. Typically, once the ESR requirement is satisfied the capacitance is adequate for filtering and has the required RMS current rating.
Manufacturers such as Nichicon, Nippon Chemi-con and Sanyo should be considered for high performance throughhole capacitors. The OS-CON (organic semicon­ductor dielectric) capacitor available from Sanyo has the lowest product of ESR and size of any aluminum electro­lytic at a somewhat higher price. An additional ceramic capacitor in parallel with OS-CON capacitors is recom­mended to reduce the effect of their lead inductance.
In surface mount applications, multiple capacitors placed in parallel may be required to meet the ESR, RMS current handling and load step requirements. Dry tantalum, spe­cial polymer and aluminum electrolytic capacitors are available in surface mount packages. Special polymer capacitors offer very low ESR but have lower capacitance density than other types. Tantalum capacitors have the highest capacitance density but it is important to only use types that have been surge tested for use in switching power supplies. Several excellent surge-tested choices are the AVX TPS and TPSV or the KEMET T510 series. Aluminum electrolytic capacitors have significantly higher ESR, but can be used in cost-driven applications providing that consideration is given to ripple current ratings and long term reliability. Other capacitor types include Panasonic SP and Sanyo POSCAPs.
Output Voltage
The LTC3703 output voltage is set by a resistor divider according to the following formula:
R
1
VV
=+
OUT
08 1
.
⎜ ⎝
⎞ ⎟
R
2
The external resistor divider is connected to the output as shown in the Functional Diagram, allowing remote voltage
sensing. The resultant feedback signal is compared with the internal precision 800mV voltage reference by the error amplifier. The internal reference has a guaranteed tolerance of ±1%. Tolerance of the feedback resistors will add additional error to the output voltage. 0.1% to 1% resistors are recommended.
MOSFET Driver Supplies (DRVCC and BOOST)
The LTC3703 drivers are supplied from the DRV
CC
and BOOST pins (see Figure 3), which have an absolute maximum voltage of 15V. If the main supply voltage, V
IN
, is higher than 15V a separate supply with a voltage between 9V and 15V must be used to power the drivers. If a separate supply is not available, one can easily be generated from the main supply using one of the circuits shown in Figure 10. If the output voltage is between 10V and 15V, the output can be used to directly power the drivers as shown in Figure 10a. If the output is below 10V, Figure 10b shows an easy way to boost the supply voltage to a sufficient level. This boost circuit uses the LT1613 in a ThinSOT area (<0.2 in
TM
package and a chip inductor for minimal extra
2
). Two other possible schemes are an extra winding on the inductor (Figure 10c) or a capacitive charge pump (Figure 10d). All the circuits shown in Figure 10 require a start-up circuit (Q1, D1 and R1) to provide driver power at initial start-up or following a short­circuit. The resistor R1 must be sized so that it supplies sufficient base current and zener bias current at the lowest expected value of V
. When using an existing supply, the
IN
supply must be capable of supplying the required gate driver current which can be estimated from:
DRVCC
= (f)(Q
I
This equation for I
G(TOP)
DRVCC
+ Q
G(BOTTOM)
)
is also useful for properly sizing
the circuit components shown in Figure 10.
An external bootstrap capacitor, CB, connected to the BOOST pin supplies the gate drive voltage for the topside MOSFETs. Capacitor C diode, D
, from the DRVCC supply when SW is low. When
B
the top side MOSFET is turned on, the driver places the C
is charged through external
B
B
voltage across the gate-source of the top MOSFET. The switch node voltage, SW, rises to V
and the BOOST pin
IN
follows. With the topside MOSFET on, the boost voltage
16
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APPLICATIO S I FOR ATIO
LTC3703
V
IN
+
1µF
+
C
IN
V
IN
LTC3703
TG
V
CC
DRV
SW
CC
BG
BGRTN
L1
Figure 10a. VCC Generated from 10V < V
V
IN
+
C
IN
N
1
R1
R2
OPTIONAL V CONNECTION 10V < V
SEC
LTC3703
V
CC
DRV
CC
FCB
GND
CC
< 15V
BGRTN
V
TG1
SW
BG1
IN
12V
C10 1µF 16V
L1
(<40V)
D2
ZHCS400
R17 1M 1%
R17 110k 1%
BAT85
V
IN
+
C
12V
LTC3703
V
OUT
10V TO 15V
+
C
OUT
3703 F10a
< 15V
OUT
12V
V
SEC
+
1µF
T1
V
OUT
+
C
OUT
3703 F10c
V
CC
DRV
CC
IN
V
IN
TG
SW
BG
BGRTN
Figure 10b. VCC Generated from V
V
IN
+
1µF
+
C
IN
V
IN
LTC3703
TG
V
CC
DRV
CC
SW
BG
BGRTN
SW
FB
12V
VN2222LL
L1
L2
10µH
LT1613
GND
+
OUT
0.22µF
V
IN
SHDN
C
OUT
< 10V
C9
4.7µF
6.3V
V
OUT
<10V
3703 F10b
BAT85
BAT85
V
OUT
+
C
OUT
3703 F10d
Figure 10c. Secondary Output Loop and VCC Connection Figure 10d. Capacitive Charge Pump for VCC (VIN < 40V)
is above the input supply: V value of the boost capacitor C of the total input capacitance of the top side MOSFET(s). The reverse breakdown of the external diode, D greater than V
IN(MAX)
. Another important consideration for the external diode is the reverse recovery and reverse leakage, either of which may cause excessive reverse current to flow at full reverse voltage. If the reverse current times reverse voltage exceeds the maximum
= VIN + V
BOOST
needs to be 100 times that
B
DRVCC
, must be
B
. The
allowable power dissipation, the diode may be damaged. For best results, use an ultrafast recovery silicon diode such as the BAS19.
An internal undervoltage lockout (UVLO) monitors the voltage on DRV cient gate drive voltage. If the DRV
to ensure that the LTC3703 has suffi-
CC
voltage falls below
CC
the UVLO threshold, the LTC3703 shuts down and the gate drive outputs remain low.
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Bottom MOSFET Source Supply (BGRTN)
The bottom gate driver, BG, switches from DRV
to BGRTN
CC
where BGRTN can be a voltage between ground and –5V. Why not just keep it simple and always connect BGRTN to ground? In high voltage switching converters, the switch node dV/dt can be many volts/ns, which will pull up on the gate of the bottom MOSFET through its Miller capacitance. If this Miller current, times the internal gate resistance of the MOSFET plus the driver resistance, exceeds the thresh­old of the FET, shoot-through will occur. By using a nega­tive supply on BGRTN, the BG can be pulled below ground when turning the bottom MOSFET off. This provides a few extra volts of margin before the gate reaches the turn-on threshold of the MOSFET. Be aware that the maximum voltage difference between DRV for example, V DRV
pin is now 13V instead of 15V.
CC
= –2V, the maximum voltage on
BGRTN
and BGRTN is 15V. If,
CC
Current Limit Programming
Programming current limit on the LTC3703 is straight forward. The I
pin sets the current limit by setting the
MAX
maximum allowable voltage drop across the bottom MOSFET. The voltage across the MOSFET is set by its on­resistance and the current flowing in the inductor, which is the same as the output current. The LTC3703 current limit circuit inverts the negative voltage across the MOSFET before comparing it to the voltage at I
, allowing the
MAX
current limit to be set with a positive voltage.
To set the current limit, calculate the expected voltage drop across the bottom MOSFET at the maximum desired current and maximum junction temperature:
= (I
V
PROG
where V
δ
is explained in the MOSFET Selection section.
is then programmed at the I
PROG
LIMIT
)(R
DS(ON)
)(
1 + δ
)
pin using the
MAX
internal 12µA pull-up and an external resistor:
R
IMAX
= V
PROG
/12µA
The current limit value should be checked to ensure that I
LIMIT(MIN)
> I
OUT(MAX)
and also that I
LIMIT(MAX)
is less than the maximum rated current of the inductor and bottom MOSFET. The minimum value of current limit generally occurs with the largest VIN at the highest ambient tem­perature, conditions that cause the largest power loss in
the converter. Note that it is important to check for self­consistency between the assumed MOSFET junction tem­perature and the resulting value of I
which heats the
LIMIT
MOSFET switches.
Caution should be used when setting the current limit based upon the R
of the MOSFETs. The maximum
DS(ON)
current limit is determined by the minimum MOSFET on­resistance. Data sheets typically specify nominal and maximum values for R reasonable assumption is that the minimum R
, but not a minimum. A
DS(ON)
DS(ON)
lies the same amount below the typical value as the maximum lies above it. Consult the MOSFET manufacturer for further guidelines.
For best results, use a V
voltage between 100mV and
PROG
500mV. Values outside of this range may give less accu­rate current limit. The current limit can also be disabled by floating the I
MAX
pin.
FEEDBACK LOOP/COMPENSATION
Feedback Loop Types
In a typical LTC3703 circuit, the feedback loop consists of the modulator, the external inductor, the output capacitor and the feedback amplifier with its compensation network. All of these components affect loop behavior and must be accounted for in the loop compensation. The modulator consists of the internal PWM generator, the output MOSFET drivers and the external MOSFETs themselves. From a feedback loop point of view, it looks like a linear voltage transfer function from COMP to SW and has a gain roughly equal to the input voltage. It has fairly benign AC behavior at typical loop compensation frequencies with significant phase shift appearing at half the switching frequency.
The external inductor/output capacitor combination makes a more significant contribution to loop behavior. These components cause a second order LC roll off at the output, with the attendant 180° phase shift. This rolloff is what filters the PWM waveform, resulting in the desired DC output voltage, but the phase shift complicates the loop compensation if the gain is still higher than unity at the pole frequency. Eventually (usually well above the LC pole frequency), the reactance of the output capacitor will approach its ESR and the rolloff due to the capacitor
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GAIN (dB)
3703 F13
0
PHASE
–6dB/OCT
–6dB/OCT
GAIN
PHASE (DEG)
FREQ
–90
–180
–270
–360
R
B
V
REF
R1
R2
FB
C2
IN
OUT
+
C1
APPLICATIO S I FOR ATIO
PHASE (DEG)
GAIN (dB)
GAIN
A
V
0
PHASE
–12dB/OCT
–6dB/OCT
FREQ
–90
–180
–270
–360
3703 F11
LTC3703
Figure 11. Transfer Function of Buck Modulator
will stop, leaving 6dB/octave and 90° of phase shift (Figure 11).
So far, the AC response of the loop is pretty well out of the user’s control. The modulator is a fundamental piece of the LTC3703 design and the external L and C are usually chosen based on the regulation and load current require­ments without considering the AC loop response. The feedback amplifier, on the other hand, gives us a handle with which to adjust the AC response. The goal is to have 180° phase shift at DC (so the loop regulates) and some­thing less than 360° phase shift at the point that the loop gain falls to 0dB. The simplest strategy is to set up the feedback amplifier as an inverting integrator, with the 0dB frequency lower than the LC pole (Figure 12). This “Type
PHASE (DEG)
IN
R1
FB
R
B
V
REF
C1
GAIN (dB)
0
OUT
+
PHASE
GAIN
–6dB/OCT
FREQ
–90
–180
–270
–360
3703 F12
Figure 12. Type 1 Schematic and Transfer Function
1” configuration is stable but transient response is less than exceptional if the LC pole is at a low frequency.
Figure 13 shows an improved “Type 2” circuit that uses an additional pole-zero pair to temporarily remove 90° of phase shift. This allows the loop to remain stable with 90° more phase shift in the LC section, provided the loop reaches 0dB gain near the center of the phase “bump.” Type 2 loops work well in systems where the ESR zero in
Figure 13. Type 2 Schematic and Transfer Function
the LC roll-off happens close to the LC pole, limiting the total phase shift due to the LC. The additional phase compensation in the feedback amplifier allows the 0dB point to be at or above the LC pole frequency, improving loop bandwidth substantially over a simple Type 1 loop. It has limited ability to compensate for LC combinations where low capacitor ESR keeps the phase shift near 180° for an extended frequency range. LTC3703 circuits using conventional switching grade electrolytic output capaci­tors can often get acceptable phase margin with Type 2 compensation.
“Type 3” loops (Figure 14) use two poles and two zeros to obtain a 180° phase boost in the middle of the frequency band. A properly designed Type 3 circuit can maintain acceptable loop stability even when low output capacitor ESR causes the LC section to approach 180° phase shift well above the initial LC roll-off. As with a Type 2 circuit, the loop should cross through 0dB in the middle of the phase bump to maximize phase margin. Many LTC3703 circuits using low ESR tantalum or OS-CON output capaci­tors need Type 3 compensation to obtain acceptable phase margin with a high bandwidth feedback loop.
IN
C3
R1
R3
FB
R
B
V
REF
C2
C1
R2
OUT
GAIN (dB)
GAIN
0
–6dB/OCT
+6dB/OCT –6dB/OCT
+
Figure 14. Type 3 Schematic and Transfer Function
PHASE
PHASE (DEG)
FREQ
–90
–180
–270
–360
3703 F14
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Feedback Component Selection
Selecting the R and C values for a typical Type 2 or Type 3 loop is a nontrivial task. The applications shown in this data sheet show typical values, optimized for the power components shown. They should give acceptable perfor­mance with similar power components, but can be way off if even one major power component is changed signifi­cantly. Applications that require optimized transient re­sponse will require recalculation of the compensation values specifically for the circuit in question. The underly­ing mathematics are complex, but the component values can be calculated in a straightforward manner if we know the gain and phase of the modulator at the crossover frequency.
Modulator gain and phase can be measured directly from a breadboard or can be simulated if the appropriate parasitic values are known. Measurement will give more accurate results, but simulation can often get close enough to give a working system. To measure the modulator gain and phase directly, wire up a breadboard with an LTC3703 and the actual MOSFETs, inductor and input and output capacitors that the final design will use. This breadboard should use appropriate construction techniques for high speed analog circuitry: bypass capacitors located close to the LTC3703, no long wires connecting components, appropriately sized ground returns, etc. Wire the feedback amplifier as a simple Type 1 loop, with a 10k resistor from V
to FB and a 0.1µF feedback capacitor from COMP to
OUT
FB. Choose the bias resistor (RB) as required to set the desired output voltage. Disconnect RB from ground and connect it to a signal generator or to the source output of a network analyzer to inject a test signal into the loop. Measure the gain and phase from the COMP pin to the output node at the positive terminal of the output capaci­tor. Make sure the analyzer’s input is AC coupled so that the DC voltages present at both the COMP and V don’t corrupt the measurements or damage the analyzer.
If breadboard measurement is not practical, a SPICE simulation can be used to generate approximate gain/ phase curves. Plug the expected capacitor, inductor and MOSFET values into the following SPICE deck and gener­ate an AC plot of V(V V
in degrees. Refer to your SPICE manual for details of
OUT
how to generate this plot.
)/V(COMP) in dB and phase of
OUT
OUT
nodes
*3703 modulator gain/phase *2003 Linear Technology *this file written to run with PSpice 8.0 *may require modifications for other SPICE simulators
*MOSFETs rfet mod sw 0.02 ;MOSFET rdson
*inductor lext sw out1 10u ;inductor value rl out1 out 0.015 ;inductor series R
*output cap cout out out2 540u ;capacitor value resr out2 0 0.01 ;capacitor ESR
*3703 internals emod mod 0 value = {57*v(comp)}
;3703multiplier vstim comp 0 0 ac 1 ;ac stimulus .ac dec 100 1k 1meg .probe .end
With the gain/phase plot in hand, a loop crossover fre­quency can be chosen. Usually the curves look something like Figure 11. Choose the crossover frequency in the rising or flat parts of the phase curve, beyond the external LC poles. Frequencies between 10kHz and 50kHz usually work well. Note the gain (GAIN, in dB) and phase (PHASE, in degrees) at this point. The desired feedback amplifier gain will be -GAIN to make the loop gain at 0dB at this frequency. Now calculate the needed phase boost, assum­ing 60° as a target phase margin:
BOOST = –(PHASE + 30°)
If the required BOOST is less than 60°, a Type 2 loop can be used successfully, saving two external components. BOOST values greater than 60° usually require Type 3 loops for satisfactory performance.
Finally, choose a convenient resistor value for R1 (10k is usually a good value). Now calculate the remaining values:
(K is a constant used in the calculations)
f = chosen crossover frequency
G = 10 absolute gain)
(GAIN/20)
(this converts GAIN in dB to G in
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LTC3703
TYPE 2 Loop:
BOOST
tan
K
=+°
2
=
2
C
21
=
12 1
CCK
=
2
R
21
=
R
B
VV
1
•• • •
π
fGKR
2
()
K
••
π
fC
()
REF
1
VR
OUT REF
45
⎞ ⎟
TYPE 3 Loop:
BOOST
K
2
C
12 1
CCK
2
R
3
R
3
C
R
B
2
=+°
tan
4
=
=
=
=
=
=
1
21
•• •
fGR
π
()
K
••
21
π
fC
1
R
1
K
1
π
23
fKR
()
1
VR
REF
VV
OUT REF
45
⎞ ⎟
section. An example of a boost converter circuit is shown in the Typical Applications section. To operate the LTC3703 in boost mode, the INV pin should be tied to the V
CC
voltage (or a voltage above 2V). Note that in boost mode, pulse-skip operation and the line feedforward compensa­tion are disabled. For a boost converter, the duty cycle of the main switch is:
VV
OUT IN
D
=
V
OUT
For high V
to VIN ratios, the maximum V
OUT
is limited
OUT
by the LTC3703’s maximum duty cycle which is typically 93%. The maximum output voltage is therefore:
V
()
V
OUT MAX
IN MIN
= 114
D
MAX
V
IN MIN()
()
Boost Converter: Inductor Selection
In a boost converter, the average inductor current equals the average input current. Thus, the maximum average inductor current can be calculated from:
I
()
LMAX
I
()
OMAX
D
−=1
MAX
I
()
OMAX
= V
V
O
IN MIN
()
Similar to a buck converter, choose the ripple current to be 20% to 40% of I
. The ripple current amplitude then
L(MAX)
determines the inductor value as follows:
V
IN MIN
=
()
If
L
D
MAX
L
The minimum required saturation current for the inductor is:
I
L(SAT)
> I
L(MAX)
+ ∆IL/2
Boost Converter Design
The following sections discuss the use of the LTC3703 as a step-up (boost) converter. In boost mode, the LTC3703 can step-up output voltages as high as 80V. These sec­tions discuss only the design steps specific to a boost converter. For the design steps common to both a buck and a boost, see the applicable section in the buck mode
Boost Converter: Power MOSFET Selection
For information about choosing power MOSFETs for a boost converter, see the Power MOSFET Selection section for the buck converter, since MOSFET selection is similar. However, note that the power dissipation equations for the MOSFETs at maximum output current in a boost converter are:
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2
PD
=
MAIN MAX
⎜ ⎝
1
V
OUT
21
⎡ ⎢
VV V
CC TH IL TH IL
P
SYNC
=
1
I
1
2
⎜ ⎝
11
1
D
MAX
MAX
D
MAX
I
MAX
1
+
R
δ
()
⎟ ⎠
RC
DR MILLER
()( )
D
MAX
()
DS ON
+
() ()
IR
MAX DS ON
()
⎟ ⎠
f
()
2
1
+
δ
()
+
()
Boost Converter: Output Capacitor Selection
In boost mode, the output capacitor requirements are more demanding due to the fact that the current waveform is pulsed instead of continuous as in a buck converter. The choice of component(s) is driven by the acceptable ripple voltage which is affected by the ESR, ESL and bulk capacitance as shown in Figure 15. The total output ripple voltage is:
VI
=+
OUT O MAX
()
1
•–
fC
OUT MAX
1
ESR
D
⎞ ⎟
where the first term is due to the bulk capacitance and second term due to the ESR.
V
COUT
V
OUT
(AC)
V
ESR
Figure 15. Output Voltage Ripple Waveform for a Boost Converter
RINGING DUE TO TOTAL INDUCTANCE (BOARD + CAP)
The choice of output capacitor is driven also by the RMS ripple current requirement. The RMS ripple current is:
II
RMS COUT O MAX
()()
O IN MIN
V
IN MIN
()
()
VV
At lower output voltages (less than 30V), it may be possible to satisfy both the output ripple voltage and RMS ripple current requirements with one or more capacitors of a single capacitor type. However, at output voltages above 30V where capacitors with both low ESR and high bulk capacitance are hard to find, the best approach is to use a combination of aluminum and ceramic capacitors (see
discussion in Input Capacitor section for the buck con­verter). With this combination, the ripple voltage can be improved significantly. The low ESR ceremic capacitor will minimize the ESR step, while the electrolytic will supply the required bulk capacitance.
Boost Converter: Input Capacitor Selection
The input capacitor of a boost converter is less critical than the output capacitor, due to the fact that the inductor is in series with the input and the input current waveform is continuous. The input voltage source impedance deter­mines the size of the input capacitor, which is typically in the range of 10µF to 100µF. A low ESR capacitor is recommended though not as critical as for the output capacitor.
The RMS input capacitor ripple current for a boost con­verter is:
I
RMS CIN
.•
()
Lf
D
= 03
MAX()
V
IN MIN
Please note that the input capacitor can see a very high surge current when a battery is suddenly connected to the input of the converter and solid tantalum capacitors can fail catastrophically under these conditions. Be sure to
specify surge-tested capacitors!
Boost Converter: Current Limit Programming
The LTC3703 provides current limiting in boost mode by monitoring the V and comparing it to the voltage at I
of the main switch during its on-time
DS
. To set the current
MAX
limit, calculate the expected voltage drop across the MOSFET at the maximum desired inductor current and maximum junction temperature. The maximum inductor current is a function of both duty cycle and maximum load current, so the limit must be set for the maximum expected duty cycle (minimum VIN) in order to ensure that the current limit does not kick in at loads < I
I
OMAX
V
PROG
()
=+
1
V
=
V
IN MIN
D
MAX
OUT
()
R
DS ON
()
()
11δ
IR
O MAX DS ON
⎟ ⎠
•()
() ()
O(MAX)
δ
+
:
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Once V
R
IMAX
Note that in a boost mode architecture, it is only possible to provide protection for “soft” shorts where V For hard shorts, the inductor current is limited only by the input supply capability. Refer to Current Limit Program­ming for buck mode for further considerations for current limit programming.
Boost Converter: Feedback Loop/Compensation
Compensating a voltage mode boost converter is unfortu­nately more difficult than for a buck converter. This is due to an additional right-half plane (RHP) zero that is present in the boost converter but not in a buck. The additional phase lag resulting from the RHP zero is difficult if not impossible to compensate even with a Type 3 loop, so the best approach is usually to roll off the loop gain at a lower frequency than what could be achievable in buck con­verter.
A typical gain/phase plot of a voltage-mode boost con­verter is shown in Figure 16. The modulator gain and phase can be measured as described for a buck converter or can be estimated as follows:
GAIN (COMP-to-V
Dominant Pole: f
is determined, R
PROG
GAIN
(dB)
= V
PROG
/12µA
is chosen as follows:
IMAX
DC gain) = 20Log(V
OUT
V
IN
=
P
V
OUT
1
2π
LC
OUT
OUT
PHASE
(DEG)
> VIN.
2
/VIN)
Since significant phase shift begins at frequencies above the dominant LC pole, choose a crossover frequency no greater than about half this pole frequency. The gain of the compensation network should equal –GAIN at this fre­quency so that the overall loop gain is 0dB here. The compensation component to achieve this, using a Type 1 amplifier (see Figure 12), is:
G = 10
–GAIN/20
C1 = 1/(2π • f • G • R1)
Run/Soft-Start Function
The RUN/SS pin is a multipurpose pin that provide a soft­start function and a means to shut down the LTC3703. Soft-start reduces the input supply’s surge current by gradually increasing the duty cycle and can also be used for power supply sequencing.
Pulling RUN/SS below 1V puts the LTC3703 into a low quiescent current shutdown (I
50µA). This pin can be
Q
driven directly from logic as shown in Figure 17. Releasing the RUN/SS pin allows an internal 4µA current source to charge up the soft-start capacitor CSS. When the voltage on RUN/SS reaches 1V, the LTC3703 begins operating at its minimum on-time. As the RUN/SS voltage increases from 1V to 3V, the duty cycle is allowed to increase from 0% to 100%. The duty cycle control minimizes input supply inrush current and elimates output voltage over­shoot at start-up and ensures current limit protection even with a hard short. The RUN/SS voltage is internally clamped at 4V.
GAIN
A
V
00
PHASE
Figure 16. Transfer Function of Boost Modulator
–12dB/OCT
–90
–180
3703 F16
RUN/SS
2V/DIV
V
OUT
5V/DIV
I
L
2A/DIV
= 50V
V
IN
= 2A
I
LOAD
= 0.01µF
C
SS
Figure 17. LTC3703 Startup Operation
2ms/DIV
3703 F17
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VV
R
R
SEC MIN()
. +
⎛ ⎝
⎞ ⎠
08 1
1 2
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If RUN/SS starts at 0V, the delay before starting is approxi­mately:
V
t
DELAY START SS SS,
1
CsFC
A
µ
4
(. / )=
025
plus an additional delay, before the output will reach its regulated value, of:
t
DELAY REG SS SS,
VV
CsFC
µ
4
A
(. / )
05
31
The start delay can be reduced by using diode D1 in Figure 18.
3.3V
OR 5V
RUN/SS
D1
C
SS
Figure 18. RUN/SS Pin Interfacing
RUN/SS
C
SS
3703 F18
MODE/SYNC Pin (Operating Mode and Secondary Winding Control)
The MODE/SYNC pin is a dual function pin that can be used for enabling or disabling Pulse Skip Mode operation and also as an external clock input for synchronizing the internal oscillator (see next section). Pulse Skip Mode is enabled when the MODE/SYNC pin is above 0.8V and is disabled, i.e. forced continuous, when the pin is below
0.8V.
In addition to providing a logic input to force continuous operation and external synchronization, the MODE/SYNC pin provides a means to regulate a flyback winding output as shown in Figure 10c. The auxiliary output is taken from a second winding on the core of the inductor, converting it to a transformer. The auxiliary output voltage is set by the main output voltage and the turns ratio of the extra winding to the primary winding as follows:
V
(N + 1)V
SEC
OUT
Since the secondary winding only draws current when the synchronous switch is on, load regulation at the auxiliary output will be relatively good as long as the main output is running in continuous mode. As the load on the primary output drops and the LTC3703 switches to Pulse Skip Mode operation, the auxiliary output may not be able to maintain regulation, especially if the load on the auxiliary
output remains heavy. To avoid this, the auxiliary output voltage can be divided down with a conventional feedback resistor string with the divided auxiliary output voltage fed back to the MODE/SYNC pin. The MODE/SYNC threshold is trimmed to 800mV with 20mV of hysteresis, allowing precise control of the auxiliary voltage and is set as follows:
where R1 and R2 are shown in Figure 10c.
If the LTC3703 is operating in Pulse Skip Mode and the auxiliary output voltage drops below V
SEC(MIN)
, the MODE/ SYNC pin will trip and the LTC3703 will resume continu­ous operation regardless of the load on the main output. Thus, the MODE/SYNC pin removes the requirement that power must be drawn from the inductor primary in order to extract power from the auxiliary winding. With the loop in continuous mode (MODE/SYNC < 0.8V), the auxiliary outputs may nominally be loaded without regard to the primary output load.
The following table summarizes the possible states avail­able on the MODE/SYNC pin:
Table 1.
MODE/SYNC Pin Condition
DC Voltage: 0V to 0.75V Forced Continuous
Current Reversal Enabled
DC Voltage: 0.87V Pulse Skip Mode Operation
No Current Reversal
Feedback Resistors Regulating a Secondary Winding Ext. Clock: 0V to 2V Forced Continuous
Current Reversal Enabled
MODE/SYNC Pin (External Synchronization)
The internal LTC3703 oscillator can be synchronized to an external oscillator by applying and clocking the MODE/ SYNC pin with a signal above 2V
. The internal oscillator
P-P
locks to the external clock after the second clock transition is received. When external synchronization is detected, LTC3703 will operate in forced continuous mode. If an external clock transition is not detected for three succes­sive periods, the internal oscillator will revert to the frequency programmed by the R
resistor. The internal
SET
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oscillator can synchronize to frequencies between 100kHz and 600kHz, independent of the frequency programmed by the R R
SET
grammed by the R frequency of the external clock. In this way, the best converter operation (ripple, component stress, etc) is achieved if the external clock signal is lost.
Fault Conditions: Output Overvoltage Protection (Crowbar)
The output overvoltage crowbar is designed to blow a system fuse in the input lead when the output of the regulator rises much higher than nominal levels. This condition causes huge currents to flow, much greater than in normal operation. This feature is designed to protect against a shorted top MOSFET; it does not protect against a failure of the controller itself.
The comparator (MAX in the Functional Diagram) detects overvoltage faults greater than 5% above the nominal output voltage. When this condition is sensed the top MOSFET is turned off and the bottom MOSFET is forced on. The bottom MOSFET remains on continuously for as long as the 0V condition persists; if V level, normal operation automatically resumes.
Minimum On-Time Considerations (Buck Mode)
Minimum on-time t that the LTC3703 is capable of turning the top MOSFET on and off again. It is determined by internal timing delays and the amount of gate charge required to turn on the top MOSFET. Low duty cycle applications may approach this minimum on-time limit and care should be taken to ensure that:
t
ON
where t
If the duty cycle falls below what can be accommodated by the minimum on-time, the LTC3703 will begin to skip cycles. The output will be regulated, but the ripple current and ripple voltage will increase. If lower frequency opera­tion is acceptable, the on-time can be increased above t
ON(MIN)
resistor. However, it is recommended that an
SET
resistor be chosen such that the frequency pro-
resistor is close to the expected
SET
returns to a safe
OUT
ON(MIN)
V
OUT
=>
Vf
IN
ON(MIN)
t
ON MIN
is typically 200ns.
is the smallest amount of time
()
for the same step-down ratio.
Pin Clearance/Creepage Considerations
The LTC3703 is available in two packages (GN16 and G28) both with identical functionality. The GN16 package gives the smallest size solution, however the 0.013” (minimum) space between pins may not provide sufficient PC board trace clearance between high and low voltage pins in higher voltage applications. Where clearance is an issue, the G28 package should be used. The G28 package has 4 unconnected pins between the all adjacent high voltage and low voltage pins, providing 5(0.0106”) = 0.053” clearance which will be sufficient for most applications up to 100V. For more information, refer to the printed circuit board design standards described in IPC-2221 (www.ipc.org).
Efficiency Considerations
The efficiency of a switching regulator is equal to the output power divided by the input power (x100%). 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. It is often useful to analyze the individual losses to determine what is limiting the efficiency and what change would produce the most improvement. Al­though all dissipative elements in the circuit produce losses, four main sources usually account for most of the losses in LTC3703 circuits: 1) LTC3703 VCC current, 2) MOSFET gate current, 3) I
2
R losses, 4) Topside MOSFET
transition losses.
Supply current. The VCC current is the DC supply
1. V
CC
current given in the Electrical Characteristics table which powers the internal control circuitry of the LTC3703. Total supply current is typically about 2.5mA and usually results in a small (<1%) loss which is proportional to V
2. DRV
current is MOSFET driver current. This current
CC
CC
.
results from switching the gate capacitance of the power MOSFETs. Each time a MOSFET gate is switched on and then off, a packet of gate charge QG moves from DRVCC to ground. The resulting dQ/dt is a current out of the DRV supply. In continuous mode, I where Q
G(TOP)
and Q
are the gate charges of the top
G(BOT)
DRVCC
= f(Q
G(TOP)
+ Q
G(BOT)
CC
),
and bottom MOSFETs.
3703fa
25
LTC3703
U
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APPLICATIO S I FOR ATIO
3. I2R losses are predicted from the DC resistances of MOSFETs, the inductor and input and output capacitor ESR. In continuous mode, the average output current flows through L but is “chopped” between the topside MOSFET and the synchronous MOSFET. If the two MOSFETs have approximately the same R resistance of one MOSFET can simply be summed with the DCR resistance of L to obtain I each R tance is 50m. This results in losses ranging from 1% to 5% as the output current increases from 1A to 5A for a 5V output.
4. Transition losses apply only to the topside MOSFET in buck mode and they become significant when operating at higher input voltages (typically 20V or greater). Transition losses can be estimated from the second term of the P equation found in the Power MOSFET Selection section.
The transition losses can become very significant at the high end of the LTC3703 operating voltage range. To improve efficiency, one may consider lowering the fre­quency and/or using MOSFETs with lower C expense of higher R
Other losses including C losses, Schottky conduction losses during dead-time, and inductor core losses generally account for less than 2% total additional loss.
Transient Response
Due to the high gain error amplifier and line feedforward compensation of the LTC3703, the output accuracy due to DC variations in input voltage and output load current will be almost negligible. For the few cycles following a load transient, however, the output deviation may be larger while the feedback loop is responding. Consider a typical 48V input to 5V output application circuit, subjected to a 1A to 5A load transient. Initially, the loop is in regulation and the DC current in the output capacitor is zero. Sud­denly, an extra 4A (= 5A-1A) flows out of the output capacitor while the inductor is still supplying only 1A. This sudden change will generate a (4A) • (R at the output; with a typical 0.015 output capacitor ESR, this is a 60mV step at the output.
= 25m and RL = 25m, then total resis-
DS(ON)
DS(ON)
2
R losses. For example, if
.
and C
IN
ESR dissipative
OUT
ESR
, then the
DS(ON)
at the
RSS
) voltage step
MAIN
The feedback loop will respond and will move at the band­width allowed by the external compensation network towards a new duty cycle. If the unity gain crossover fre­quency is set to 50kHz, the COMP pin will get to 60% of the way to 90% duty cycle in 3µs. Now the inductor is seeing 43V across itself for a large portion of the cycle and its current will increase from 1A at a rate set by di/dt = V/L. If the inductor value is 10µH, the peak di/dt will be 43V/10µH or 4.3A/µs. Sometime in the next few micro-seconds after the switch cycle begins, the inductor current will have risen to the 5A level of the load current and the output voltage will stop dropping. At this point, the inductor cur­rent will rise somewhat above the level of the output cur­rent to replenish the charge lost from the output capacitor during the load transient. With a properly compensated loop, the entire recovery time will be inside of 10µs.
Most loads care only about the maximum deviation from ideal, which occurs somewhere in the first two cycles after the load step hits. During this time, the output capacitor does all the work until the inductor and control loop regain control. The initial drop (or rise if the load steps down) is entirely controlled by the ESR of the capacitor and amounts to most of the total voltage drop. To minimize this drop, choose a low ESR capacitor and/or parallel multiple ca­pacitors at the output. The capacitance value accounts for the rest of the voltage drop until the inductor current rises. With most output capacitors, several devices paralleled to get the ESR down will have so much capacitance that this drop term is negligible. Ceramic capacitors are an excep­tion; a small ceramic capacitor can have suitably low ESR with relatively small values of capacitance, making this second drop term more significant.
Optimizing Loop Compensation
Loop compensation has a fundamental impact on tran­sient recovery time, the time it takes the LTC3703 to recover after the output voltage has dropped due to a load step. Optimizing loop compensation entails maintaining the highest possible loop bandwidth while ensuring loop stability. The feedback component selection section de­scribes in detail the techniques used to design an opti­mized Type 3 feedback loop, appropriate for most LTC3703 systems.
26
3703fa
LTC3703
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APPLICATIO S I FOR ATIO
Measurement Techniques
Measuring transient response presents a challenge in two respects: obtaining an accurate measurement and gener­ating a suitable transient to test the circuit. Output mea­surements should be taken with a scope probe directly across the output capacitor. Proper high frequency prob­ing techniques should be used. In particular, don’t use the 6" ground lead that comes with the probe! Use an adapter that fits on the tip of the probe and has a short ground clip to ensure that inductance in the ground path doesn’t cause a bigger spike than the transient signal being measured. Conveniently, the typical probe tip ground clip is spaced just right to span the leads of a typical output capacitor.
Now that we know how to measure the signal, we need to have something to measure. The ideal situation is to use the actual load for the test and switch it on and off while watching the output. If this isn’t convenient, a current step generator is needed. This generator needs to be able to turn on and off in nanoseconds to simulate a typical switching logic load, so stray inductance and long clip leads between the LTC3703 and the transient generator
LTC3703
PULSE
GENERATOR
0V TO 10V
100Hz, 5%
DUTY CYCLE
LOCATE CLOSE TO THE OUTPUT
Figure 19. Transient Load Generator
50
must be minimized.
Figure 19 shows an example of a simple transient genera­tor. Be sure to use a noninductive resistor as the load element—many power resistors use an inductive spiral pattern and are not suitable for use here. A simple solution is to take ten 1/4W film resistors and wire them in parallel to get the desired value. This gives a noninductive resistive load which can dissipate 2.5W continuously or 50W if pulsed with a 5% duty cycle, enough for most LTC3703 circuits. Solder the MOSFET and the resistor(s) as close to the output of the LTC3703 circuit as possible and set up
V
OUT
R
LOAD
IRFZ44 OR EQUIVALENT
3703 F19
the signal generator to pulse at a 100Hz rate with a 5% duty cycle. This pulses the LTC3703 with 500µs transients10ms apart, adequate for viewing the entire transient recovery time for both positive and negative transitions while keep­ing the load resistor cool.
Design Example
As a design example, take a supply with the following specifications: V 12V ±5%, I
OUT(MAX)
= 36V to 72V (48V nominal), V
IN
= 10A, f=250kHz. First, calculate R
OUT
SET
=
to give the 250kHz operating frequency:
R
= 7100/(250-25) = 31.6k
SET
Next, choose the inductor value for about 40% ripple current at maximum V
V
L
250 0 4 10
( )( . )( )
12
kHz A
IN
:
12
⎛ ⎜
1
⎟ ⎠
72
H=
10
With 10µH inductor, ripple current will vary from 3.2A to 4A (32% to 40%) over the input supply range.
Next, verify that the minimum on-time is not violated. The minimum on-time occurs at maximum VIN:
t
()
ON MIN
V
OUT
== =
V f kHz
IN MIN
() ( )
()
12
72 250
667
ns
which is above the LTC3703’s 200ns minimum on-time.
Next, choose the top and bottom MOSFET switch. Since the drain of each MOSFET will see the full supply voltage 72V(max) plus any ringing, choose a 100V MOSFET to provide a margin of safety. Si7456DP has a 100V BV R
= 25mΩ(max), δ = 0.009/°C, C
DS(ON)
10nC)/50V = 180pF, V
GS(MILLER)
= 4.7V, θJA = 20°C/W.
MILLER
= (19nC –
DSS
,
The power dissipation can be estimated at maximum input voltage, assuming a junction temperature of 100°C (30°C above an ambient of 70°C):
P
MAIN
12
=+
72
() ()( )•
+
72
070 094 164
=+=
2
() . ( – )(. )
10 1 0 009 100 25 0 025
[]
10
2
2
WWW
...
pF k
2 180
1
⎛ ⎜
10 4 7147
+
–. .
()
250
⎟ ⎠
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27
LTC3703
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APPLICATIO S I FOR ATIO
And double check the assumed TJ in the MOSFET:
= 70°C + (1.64W)(20°C/W) = 103°C
T
J
Since the synchronous MOSFET will be conducting over twice as long each period (almost 100% of the period in short circuit) as the top MOSFET, use two Si7456DP MOSFETs on the bottom:
72 12
P
SYNC
=
⎛ ⎜
⎛ ⎜
0 025
.
TJ = 70°C + (1.74W)(20°C/W) = 105°C
Next, set the current limit resistor. Since I limit should be set such that the minimum current limit is >10A. Minimum current limit occurs at maximum R Using the above calculation for bottom MOSFET T max R
Therefore, I
= (25m/2) [1 + 0.009 (105-25)] = 21.5m
DS(ON)
MAX
= 0.215V. The R
0.215V/12µA = 18kΩ.
C
is chosen for an RMS current rating of about 5A (I
IN
2) at 85°C. For the output capacitor, two low ESR OSCON capacitors (18m each) are used to minimize output voltage changes due to inductor current ripple and load steps. The ripple voltage will be:
V
OUT(RIPPLE)
= 36mV
However, a 0A to 10A load step will cause an output voltage change of up to:
2
10 1 0 009 100 25
() . ( – )•
⎟ ⎠
72
174
=
⎟ ⎠
2
+
[]
.
W
= 10A, the
MAX
.
DS(ON)
, the
J
pin voltage should be set to (10A)(0.0215)
resistor can now be chosen to be
SET
/
MAX
= ∆I
(ESR) = (4A)(0.018Ω/2)
L(MAX)
1. Keep the signal and power grounds separate. The signal ground consists of the LTC3703 GND pin, the ground return of C
, and the (–) terminal of V
VCC
. The power
OUT
ground consists of the Schottky diode anode, the source of the bottom side MOSFET, and the (–) terminal of the input capacitor and DRV
capacitor. Connect the signal
CC
and power grounds together at the (–) terminal of the output capacitor. Also, try to connect the (–) terminal of the output capacitor as close as possible to the (–) terminals of the input and DRV
capacitor and away from
CC
the Schottky loop described in (2).
2. The high di/dt loop formed by the top N-channel MOSFET, the bottom MOSFET and the C
capacitor
IN
should have short leads and PC trace lengths to minimize high frequency noise and voltage stress from inductive ringing.
3. Connect the drain of the top side MOSFET directly to the (+) plate of C MOSFET directly to the (–) terminal of C
, and connect the source of the bottom side
IN
. This capacitor
IN
provides the AC current to the MOSFETs.
4. Place the ceramic C diately next to the IC, between DRV
decoupling capacitor imme-
DRVCC
and BGRTN. This
CC
capacitor carries the MOSFET drivers’ current peaks. Likewise the C
capacitor should also be next to the IC
B
between BOOST and SW.
5. Place the small-signal components away from high frequency switching nodes (BOOST, SW, TG, and BG). In the layout shown in Figure 20, all the small signal compo­nents have been placed on one side of the IC and all of the power components have been placed on the other. This also helps keep the signal ground and power ground isolated.
V
OUT(STEP)
= ∆I
LOAD(ESR)
= (10A)(0.009Ω)
= 90mV
PC Board Layout Checklist
When laying out the printed circuit board, the following checklist should be used to ensure proper operation of the LTC3703. These items are also illustrated graphically in the layout diagram of Figure 18. For layout of a Boost Mode Converter, layout is similar with V
IN
and V
swapped.
OUT
Check the following in your layout:
28
6. A separate decoupling capacitor for the supply, VCC, is useful with an RC filter between the DRV
supply and V
CC
CC
pin to filter any noise injected by the drivers. Connect this capacitor close to the IC, between the V and keep the ground side of the V ground) isolated from the ground side of the DRV
and GND pins
CC
capacitor (signal
CC
CC
capacitor (power ground).
7. For optimum load regulation and true remote sensing, the top of the output resistor divider should connect independently to the top of the output capacitor (Kelvin
3703fa
LTC3703
U
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APPLICATIO S I FOR ATIO
connection), staying away from any high dV/dt traces. Place the divider resistors near the LTC3703 in order to keep the high impedance FB node short.
8. For applications with multiple switching power convert­ers connected to the same input supply, make sure that the input filter capacitor for the LTC3703 is not shared with
1
MODE/SYNC
R
SET
2
FSET
R
C1
C
C2
R
C2
R1
C
C3
C
C1
R
C
MAX
SS
R2
3
COMP
4
FB
5
I
6
INV
7
RUN/SS
8
GND
LTC3703
MAX
V
BOOST
TG
SW
V
CC
DRV
BG
BGRTN
16
IN
15
14
13
12
11
CC
10
9
C
VCC
X5R
other converters. AC input current from another converter could cause substantial input voltage ripple, and this could interfere with the operation of the LTC3703. A few inches of PC trace or wire (L 100nH) between CIN of the LTC3703 and the actual source V
should be sufficient to
IN
prevent input noise interference problems.
V
CC
R
F
C
DRVCC
X5R
V
IN
D
B
M1
+
C
IN
C
B
L1
+
M2
+
C
D1
OUT
V
OUT
Figure 20. LTC3703 Buck Converter Suggested Layout
3703 F18
3703fa
29
LTC3703
TYPICAL APPLICATIO S
36V-72V Input Voltage to 5V/10A Step-Down Converter with Pulse Skip Mode Enabled
U
V
CC
9.3V TO 15V
C
1000pF
R
C2
100
C 2200pF
+
22µF
R
10
C
DRVCC
10µF
25V
F
1
MODE/SYNC
R
SET
25k
2
R
C1
10k
C
C2
R2
21.5k 1%
R1 113k
C3
1%
470pF
R
0.1µF
C1
MAX
C
FSET
LTC3703
3
COMP
4
FB
20k
5
I
MAX
6
INV
SS
7
RUN/SS
8
GND
V
BOOST
SW
V
DRV
BG
BGRTN
16
IN
15
14
TG
13
12
CC
11
CC
10
9
C 1µF
D BAS19
C
0.1µF
VCC
B
B
V
IN
36V TO 72V
M1 Si7852DP
M2 Si7852DP
+
L1
4.7µH
C
IN
68µF 100V
×2
C
OUT
270µF
10V
×2
D1 MBR1100
+
3703 TA01
V 5V 10A
OUT
Single Input Supply 12V/5A Output Step-Down Converter
100
*
FZT600
10k
12V
V
IN
15V TO 80V
+
22µF
R
10
C
DRVCC
10µF
25V
F
1
25k
12k
MODE/SYNC
2
FSET
3
COMP
4
FB
5
I
MAX
6
INV
7
RUN/SS
8
GND
LTC3703
R
C
470pF
R
MAX
0.1µF
SET
C1
C
SS
R
C1
10k
C
C2
1000pF
R2
8.06k 1%
R
C2
C
C3
2200pF
R1 113k 1%
100
*OPTIONAL ZENER PROVIDES UNDERVOLTAGE LOCKOUT ON INPUT SUPPLY, V
V
BOOST
SW
V
DRV
BGRTN
TG
BG
16
IN
15
14
13
12
CC
11
CC
10
9
UVLO
D
B
BAS19
C
B
0.1µF
C
VCC
1µF
10 + V
Z
M1 Si7852DP
M2 Si7852DP
+
8µH
L1
C
IN
68µF 100V
C
OUT
270µF
16V
D1 MBR1100
+
3703 TA02
CMDSH-3
V
OUT
12V 5A
3703fa
30
PACKAGE DESCRIPTIO
U
GN Package
16-Lead Plastic SSOP (Narrow .150 Inch)
(Reference LTC DWG # 05-08-1641)
.045 ±.005
16
15
(4.801 – 4.978)
.189 – .196*
14
12 11 10
13
LTC3703
.009
(0.229)
9
REF
.254 MIN
RECOMMENDED SOLDER PAD LAYOUT
.007 – .0098
(0.178 – 0.249)
.016 – .050
NOTE:
1. CONTROLLING DIMENSION: INCHES
2. DIMENSIONS ARE IN
3. DRAWING NOT TO SCALE
*DIMENSION DOES NOT INCLUDE MOLD FLASH. MOLD FLASH SHALL NOT EXCEED 0.006" (0.152mm) PER SIDE
**DIMENSION DOES NOT INCLUDE INTERLEAD FLASH. INTERLEAD FLASH SHALL NOT EXCEED 0.010" (0.254mm) PER SIDE
(0.406 – 1.270)
(MILLIMETERS)
INCHES
.150 – .165
.0250 BSC.0165 ± .0015
.015
(0.38 ± 0.10)
0° – 8° TYP
± .004
28-Lead Plastic SSOP (5.3mm)
(Reference LTC DWG # 05-08-1640)
1.25 ±0.12
.229 – .244
(5.817 – 6.198)
× 45°
.008 – .012
(0.203 – 0.305)
G Package
.0532 – .0688
(1.35 – 1.75)
TYP
2526 22 21 20 19 181716 1523242728
12
3
9.90 – 10.50* (.390 – .413)
.150 – .157** (3.810 – 3.988)
5
4
678
.004 – .0098
(0.102 – 0.249)
.0250
(0.635)
GN16 (SSOP) 0204
BSC
7.8 – 8.2
0.42 ±0.03 0.65 BSC
RECOMMENDED SOLDER PAD LAYOUT
5.00 – 5.60** (.197 – .221)
0.09 – 0.25
(.0035 – .010)
NOTE:
1. CONTROLLING DIMENSION: MILLIMETERS
2. DIMENSIONS ARE IN
3. DRAWING NOT TO SCALE *
DIMENSIONS DO NOT INCLUDE MOLD FLASH. MOLD FLASH SHALL NOT EXCEED .152mm (.006") PER SIDE
**
DIMENSIONS DO NOT INCLUDE INTERLEAD FLASH. INTERLEAD FLASH SHALL NOT EXCEED .254mm (.010") PER SIDE
0.55 – 0.95
(.022 – .037)
MILLIMETERS
(INCHES)
5.3 – 5.7
0° – 8°
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.
12345678 9 10 11 12 1413
0.65
(.0256)
BSC
0.22 – 0.38
(.009 – .015)
TYP
(.079)
MAX
0.05
(.002)
MIN
G28 SSOP 0204
7.40 – 8.20
(.291 – .323)
2.0
3703fa
31
LTC3703
TYPICAL APPLICATIO
U
12V to 24V/5A Synchronous Boost Converter
0.1µF
R1
113k
1%
10k
R2
3.92k 1%
R
SET
C
100pF
R
MAX
C1
0.1F
C
1
MODE/SYNC
30.1k
2
FSET
3
COMP
4
FB
15k
5
I
MAX
6
INV
SS
7
RUN/SS
8
GND
L1: VISHAY IHLPSOSOEZ C
IN
16
V
IN
15
BOOST
LTC3703
: OSCON 20SP180M
SW
V
DRV
BGRTN
TG
BG
14
13
12
CC
11
CC
10
9
+
C 10µF
R
F
10
DRVCC
D
22µF 25V
B
CMDSH-3
C
B
0.1µF
C
VCC
1µF
C
: SANYO 35MV220AX
OUT1
: UNITED CHEMICON
C
OUT2
NTS60X5R1H106MT
M1 Si7892DP
M2 Si7892DP
C
OUT
220µF
35V
B240A
L1
3.3µH
100µF
16V
V
OUT
24V
C
+
×3
+
C
IN
3703 TA03
OUT2
10µF 50V X5R ×2
5A
V
IN
10V TO 15V
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up to 60V, Drivers 10,000pF Gate Capacitance, I
IN
, 3V ≤ VIN 7V, I
SENSE
6V, Current Mode, I
OUT
60V, No Protection Diode Required, 8-Lead MSOP
OUT
Single Inductor
OUT
OUT
36V
OUT
20A
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20A
20A
OUT
20A
32
Linear Technology Corporation
1630 McCarthy Blvd., Milpitas, CA 95035-7417
(408) 432-1900 ● FAX: (408) 434-0507 ● www.linear.com
3703fa
LT 0306 REV A • PRINTED IN USA
© LINEAR TECHNOLOGY CORPORATION 2003
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