LT1374CR#TRPBF [Linear]

LT1374 - 4.5A, 500kHz Step-Down Switching Regulator; Package: DD PAK; Pins: 7; Temperature Range: 0°C to 70°C;
LT1374CR#TRPBF
型号: LT1374CR#TRPBF
厂家: Linear    Linear
描述:

LT1374 - 4.5A, 500kHz Step-Down Switching Regulator; Package: DD PAK; Pins: 7; Temperature Range: 0°C to 70°C

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LT1374  
4.5A, 500kHz Step-Down  
Switching Regulator  
U
FEATURES  
DESCRIPTIO  
Constant 500kHz Switching Frequency  
TheLT®1374isa500kHzmonolithicbuckmodeswitching  
regulator. A 4.5A switch is included on the die along with  
allthenecessaryoscillator,controlandlogiccircuitry.High  
switchingfrequencyallowsaconsiderablereductioninthe  
sizeofexternalcomponents.Thetopologyiscurrentmode  
for fast transient response and good loop stability. Both  
fixed output voltage and adjustable parts are available.  
High Power 16-Pin TSSOP Package Available  
Uses All Surface Mount Components  
Inductor Size Reduced to 1.8µH  
Saturating Switch Design: 0.07Ω  
Effective Supply Current: 2.5mA  
Shutdown Current: 20µA  
Cycle-by-Cycle Current Limiting  
Easily Synchronizable  
Aspecialhighspeedbipolarprocessandnewdesigntech-  
niquesachievehighefficiencyathighswitchingfrequency.  
Efficiency is maintained over a wide output current range  
by using the output to bias the circuitry and by utilizing a  
supply boost capacitor to saturate the power switch.  
U
APPLICATIO S  
Portable Computers  
TheLT1374isavailableinstandard7-pinDD,TO-220,fused  
lead SO-8 and 16-pin exposed pad TSSOP packages. Full  
cycle-by-cycle short-circuit protection and thermal shut-  
downareprovided.Standardsurfacemountexternalparts  
may be used, including the inductor and capacitors. There  
is the optional function of shutdown or synchronization. A  
shutdownsignalreducessupplycurrentto20µA.Synchro-  
nizationallowsanexternallogiclevelsignaltoincreasethe  
Battery-Powered Systems  
Battery Chargers  
Distributed Power  
internal oscillator from 580kHz to 1MHz.  
, LTC and LT are registered trademarks of Linear Technology Corporation.  
U
TYPICAL APPLICATIO  
5V Buck Converter  
Efficiency vs Load Current  
D2  
100  
CMDSH3 OR FMMD914  
V
V
= 5V  
OUT  
IN  
= 10V  
95  
90  
85  
80  
75  
70  
L = 10µH  
C2  
0.27µF  
L1**  
5µH  
BOOST  
OUTPUT**  
5V, 4.25A  
INPUT  
V
V
IN  
SW  
6V TO 25V  
+
C3*  
LT1374-5 BIAS  
10µF TO  
50µF  
DEFAULT  
= ON  
SHDN  
SENSE  
GND  
V
C
C1  
+
D1  
100µF, 10V  
SOLID  
C
C
MBRS330T3  
1.5nF  
TANTALUM  
* RIPPLE CURRENT RATING I /2  
OUT  
1374 TA01  
0
0.5 1.0 1.5 2.0 2.5 3.0 3.5 4.0  
LOAD CURRENT (A)  
** INCREASE L1 TO 10µH FOR LOAD CURRENTS ABOVE 3.5A AND TO 20µH ABOVE 4A  
SEE APPLICATIONS INFORMATION  
1374 TA02  
1374fb  
1
LT1374  
W W U W  
ABSOLUTE AXI U RATI GS (Note 1)  
Input Voltage  
FB Pin Current (Adjustable Part)............................ 1mA  
SENSE Voltage (Fixed 5V Part) ................................. 7V  
SYNC Pin Voltage ..................................................... 7V  
Operating Junction Temperature Range  
LT1374C............................................... 0°C to 125° C  
LT1374I ........................................... 40°C to 125°C  
Storage Temperature Range ................ 65°C to 150°C  
Lead Temperature (Soldering, 10 sec)................. 300°C  
LT1374 ............................................................... 25V  
LT1374HV .......................................................... 32V  
BOOST Pin Voltage ................................................. 38V  
BOOST Pin Above Input Voltage ............................. 15V  
SHDN Pin Voltage..................................................... 7V  
BIAS Pin Voltage ...................................................... 7V  
FB Pin Voltage (Adjustable Part)............................ 3.5V  
U W  
U
PACKAGE/ORDER I FOR ATIO  
ORDER  
PART NUMBER  
ORDER  
PART NUMBER  
FRONT VIEW  
7
6
5
4
3
2
1
FB OR SENSE*  
BOOST  
LT1374CR  
LT1374CS8  
V
TAB  
IS  
IN  
LT1374CR-5  
LT1374CR-SYNC  
LT1374CS8-5  
LT1374CS8-SYNC  
GND  
GND  
V
SW  
SYNC OR SHDN*  
TOP VIEW  
V
C
LT1374CR-5 SYNC  
LT1374HVCR  
LT1374IR  
LT1374CS8-5 SYNC  
R PACKAGE  
7-LEAD PLASTIC DD  
1
2
3
4
8
7
6
5
V
V
SW  
SYNC  
OR SHDN*  
IN  
LT1374HVCS8  
LT1374IS8  
BOOST  
FB OR  
SENSE*  
TJMAX = 125°C, θJA = 30°C/ W  
V
C
WITH PACKAGE SOLDERED TO 0.5 SQUARE INCH  
COPPER AREA OVER BACKSIDE GROUND PLANE  
OR INTERNAL POWER PLANE. θJA CAN VARY  
FROM 20°C/W TO >40°C/W DEPENDING ON  
MOUNTING TECHNIQUES  
LT1374IR-5  
LT1374IS8-5  
FGND  
BIAS  
LT1374IR-SYNC  
LT1374IR-5 SYNC  
LT1374HVIR  
LT1374IS8-SYNC  
LT1374IS8-5 SYNC  
LT1374HVIS8  
S8 PACKAGE  
8-LEAD PLASTIC SO  
θJA = 80°C/ W WITH FUSED (FGND)  
GROUND PIN CONNECTED TO GROUND  
PLANE OR LARGE LANDS  
ORDER  
PART NUMBER  
S8 PART MARKING  
TOP VIEW  
1374  
13745  
1374I  
1374I5  
GND  
NC  
1
2
3
4
5
6
7
8
16  
15  
14  
13  
12  
11  
10  
9
GND  
LT1374CFE  
LT1374IFE  
V
SW  
1374SN 374ISN  
3745SN 74I5SN  
1374HV 1374HVI  
V
V
SW  
IN  
V
IN  
SYNC  
SHDN  
BOOST  
FB/SENSE  
NC  
V
C
TAB IS  
GND  
ORDER  
PART NUMBER  
FRONT VIEW  
BIAS  
GND  
FB OR SENSE*  
7
6
5
4
3
2
1
GND  
BOOST  
V
IN  
FE16 PACKAGE  
16-LEAD PLASTIC TSSOP  
LT1374CT7  
LT1374CT7-5  
LT1374IT7  
GND  
V
SW  
SHDN  
θJA = 40°C/ W  
EXPOSED PAD SOLDERED TO  
GROUND PLANE  
V
C
T7 PACKAGE  
7-LEAD PLASTIC TO-220  
LT1374IT7-5  
TJMAX = 125°C, θJA = 50°C/ W, θJC = 4°C/ W  
*Default is the adjustable output voltage device with FB pin and shutdown function. Option -5 replaces FB with SENSE pin for fixed 5V output applications.  
-SYNC replaces SHDN with SYNC pin for applications requiring synchronization. Consult LTC Marketing for parts specified with wider operating  
temperature ranges.  
1374fb  
2
LT1374  
ELECTRICAL CHARACTERISTICS  
The denotes specifications which apply over the full operating tempera-  
ture range, otherwise specifications are at TJ = 25°C. VIN = 15V, VC = 1.5V, Boost = VIN + 5V, switch open, unless otherwise noted.  
PARAMETER  
CONDITIONS  
All Conditions  
All Conditions  
MIN  
TYP  
MAX  
UNITS  
Feedback Voltage (Adjustable)  
2.39  
2.36  
2.42  
2.45  
2.48  
V
V
Sense Voltage (Fixed 5V)  
4.94  
4.90  
5.0  
5.06  
5.10  
V
V
SENSE Pin Resistance  
7
10  
14  
kΩ  
Reference Voltage Line Regulation  
5V V 25V (5V V 32V for LT1374HV)  
0.01  
0.03  
%/V  
IN  
IN  
Feedback Input Bias Current  
Error Amplifier Voltage Gain  
Error Amplifier Transconductance  
0.5  
400  
2
µA  
(Notes 2, 8)  
200  
I (V ) = ±10µA (Note 8)  
1500  
1000  
2000  
2700  
3100  
µMho  
µMho  
C
V Pin to Switch Current Transconductance  
5.3  
225  
225  
0.9  
2.1  
6
A/V  
µA  
µA  
V
C
Error Amplifier Source Current  
Error Amplifier Sink Current  
V
V
= 2.1V or V  
= 2.7V or V  
= 4.4V  
= 5.6V  
140  
140  
320  
320  
FB  
SENSE  
FB  
SENSE  
V Pin Switching Threshold  
C
Duty Cycle = 0  
V Pin High Clamp  
C
V
Switch Current Limit  
V Open, V = 2.1V or V  
C
= 4.4V, DC 50%  
4.5  
8.5  
A
FB  
SENSE  
Slope Compensation (Note 9)  
Switch On Resistance (Note 7)  
DC = 80%  
0.8  
0.07  
A
I
= 4.5A  
0.1  
SW  
0.13  
Maximum Switch Duty Cycle  
Switch Frequency  
V
FB  
= 2.1V or V  
= 4.4V  
90  
86  
93  
93  
%
%
SENSE  
V Set to Give 50% Duty Cycle  
C
460  
440  
500  
540  
560  
kHz  
kHz  
Switch Frequency Line Regulation  
Frequency Shifting Threshold on FB Pin  
Minimum Input Voltage (Note 3)  
Minimum Boost Voltage (Note 4)  
Boost Current (Note 5)  
5V V 25V, (5V V 32V for LT1374HV)  
0
0.15  
1.3  
5.5  
3.0  
%/V  
V
IN  
IN  
f = 10kHz  
0.8  
1.0  
5.0  
2.3  
V
I
4.5A  
V
SW  
I
I
= 1A  
= 4.5A  
20  
90  
35  
140  
mA  
mA  
SW  
SW  
V
Supply Current (Note 6)  
V
BIAS  
V
BIAS  
V
SHDN  
= 5V  
= 5V  
0.9  
3.2  
20  
1.4  
4.0  
mA  
mA  
IN  
BIAS Supply Current (Note 6)  
Shutdown Supply Current  
= 0V, V 25V, V = 0V, V Open  
50  
75  
µA  
µA  
IN  
SW  
C
V
= 0V, V 32V, V = 0V, V Open  
30  
75  
µA  
µA  
SHDN  
IN  
SW  
C
100  
Lockout Threshold  
V Open  
C
2.3  
2.38  
2.46  
V
Shutdown Thresholds  
V Open Device Shutting Down  
0.13  
0.25  
0.37  
0.45  
0.60  
0.7  
V
V
C
Device Starting Up  
Synchronization Threshold  
Synchronizing Range  
1.5  
2.2  
V
kHz  
kΩ  
580  
1000  
SYNC Pin Input Resistance  
40  
regulated so that the reference voltage and oscillator frequency remain  
constant. Actual minimum input voltage to maintain a regulated output will  
depend on output voltage and load current. See Applications Information.  
Note 4: This is the minimum voltage across the boost capacitor needed to  
guarantee full saturation of the internal power switch.  
Note 1: Absolute Maximum Ratings are those values beyond which the life  
of a device may be impaired.  
Note 2: Gain is measured with a V swing equal to 200mV above the  
C
switching threshold level to 200mV below the upper clamp level.  
Note 3: Minimum input voltage is not measured directly, but is guaranteed  
by other tests. It is defined as the voltage where internal bias lines are still  
1374fb  
3
LT1374  
ELECTRICAL CHARACTERISTICS  
Note 5: Boost current is the current flowing into the boost pin with the pin  
Note 8: Transconductance and voltage gain refer to the internal amplifier  
exclusive of the voltage divider. To calculate gain and transconductance,  
refer to the SENSE pin on the fixed voltage parts. Divide values shown by  
held 5V above input voltage. It flows only during switch on time.  
Note 6: V supply current is the current drawn when the BIAS pin is held  
IN  
the ratio V /2.42.  
at 5V and switching is disabled. If the BIAS pin is unavailable or open  
OUT  
circuit, the sum of V and BIAS supply currents will be drawn by the V  
Note 9: Slope compensation is the current subtracted from the switch  
current limit at 80% duty cycle. See Maximum Output Load Current in the  
Applications Information section for further details.  
IN  
IN  
pin.  
Note 7: Switch on resistance is calculated by dividing V to V voltage  
IN  
SW  
by the forced current (4.5A). See Typical Performance Characteristics for  
the graph of switch voltage at other currents.  
U W  
TYPICAL PERFOR A CE CHARACTERISTICS  
Switch Voltage Drop  
Switch Peak Current Limit  
Feedback Pin Voltage  
2.430  
2.425  
2.420  
2.415  
2.410  
6.5  
6.0  
5.5  
5.0  
4.5  
4.0  
3.5  
3.0  
500  
450  
400  
350  
300  
250  
200  
150  
100  
50  
125°C  
25°C  
TYPICAL  
MINIMUM  
40°C  
0
–25  
0
25  
50  
75  
125  
2
50  
100  
0
1
3
4
5
0
20  
80  
100  
40  
60  
DUTY CYCLE (%)  
TEMPERATURE (°C)  
SWITCH CURRENT (A)  
1374 G03  
1374 G18  
1374 G02  
Shutdown Pin Bias Current  
Standby and Shutdown Thresholds  
Shutdown Supply Current  
25  
20  
500  
400  
300  
200  
8
2.40  
2.36  
2.32  
0.8  
V
= 0V  
SHDN  
CURRENT REQUIRED TO FORCE SHUTDOWN  
(FLOWS OUT OF PIN). AFTER SHUTDOWN,  
CURRENT DROPS TO A FEW µA  
STANDBY  
15  
10  
5
START-UP  
AT 2.38V STANDBY THRESHOLD  
(CURRENT FLOWS OUT OF PIN)  
0.4  
4
SHUTDOWN  
0
0
0
0
5
10  
15  
20  
25  
50  
TEMPERATURE (°C)  
100 125  
50  
100 125  
–50 –25  
0
25  
75  
–50 –25  
0
25  
75  
INPUT VOLTAGE (V)  
JUNCTION TEMPERATURE (°C)  
1374 G06  
1374 G04  
1374 G05  
1374fb  
4
LT1374  
U W  
TYPICAL PERFOR A CE CHARACTERISTICS  
Shutdown Supply Current  
Error Amplifier Transconductance  
Error Amplifier Transconductance  
2500  
2000  
1500  
1000  
500  
70  
60  
50  
40  
30  
20  
10  
0
3000  
2500  
2000  
1500  
1000  
500  
200  
150  
100  
50  
PHASE  
V
IN  
= 25V  
GAIN  
V
IN  
= 10V  
V
C
C
OUT  
12pF  
R
OUT  
200k  
–3  
V
2 × 10  
(
)
FB  
ERROR AMPLIFIER EQUIVALENT CIRCUIT  
= 50Ω  
0
R
LOAD  
0
–50  
–50 –25  
0
25  
50  
75 100 125  
1k  
1M  
0
0.1  
0.2  
SHUTDOWN VOLTAGE (V)  
0.3  
0.4  
100  
10k 100k  
FREQUENCY (Hz)  
10M  
JUNCTION TEMPERATURE (°C)  
1374 G09  
1374 G07  
1374 G08  
Minimum Input Voltage  
with 5V Output  
Frequency Foldback  
Switching Frequency  
6.4  
6.2  
6.0  
5.8  
5.6  
5.4  
5.2  
5.0  
550  
500  
400  
300  
200  
100  
0
540  
530  
520  
510  
500  
490  
480  
470  
460  
450  
MINIMUM  
STARTING  
VOLTAGE  
SWITCHING  
FREQUENCY  
MINIMUM  
RUNNING  
VOLTAGE  
FEEDBACK PIN  
CURRENT  
1
10  
100  
1000  
–25  
0
25  
50  
75  
125  
50  
100  
0
0.5  
1.0  
1.5  
2.0  
2.5  
LOAD CURRENT (mA)  
TEMPERATURE (°C)  
FEEDBACK PIN VOLTAGE (V)  
1374 G12  
1374 G11  
1374 G10  
Maximum Load Current  
at VOUT = 10V  
Maximum Load Current  
at VOUT = 3.3V  
Maximum Load Current  
at VOUT = 5V  
4.5  
4.0  
3.5  
3.0  
4.5  
4.0  
3.5  
3.0  
4.5  
4.0  
3.5  
3.0  
L = 20µH  
V
OUT  
= 10V  
L = 20µH  
L = 20µH  
L = 10µH  
L = 10µH  
L = 10µH  
L = 5µH  
L = 5µH  
L = 5µH  
V
OUT  
= 3.3V  
5
V
OUT  
= 5V  
5
0
5
10  
INPUT VOLTAGE (V)  
15  
20  
25  
0
10  
INPUT VOLTAGE (V)  
15  
20  
25  
0
10  
15  
20  
25  
INPUT VOLTAGE (V)  
1374 G13  
1374 G14  
1374 G15  
1374fb  
5
LT1374  
U W  
TYPICAL PERFOR A CE CHARACTERISTICS  
VC Pin Shutdown Threshold  
BOOST Pin Current  
Inductor Core Loss  
100  
1.0  
0.1  
20  
12  
8
1.4  
DUTY CYCLE = 100%  
V
= 5V, V = 10V, I  
= 1A  
OUT  
SHUTDOWN  
IN  
OUT  
90  
80  
70  
60  
50  
40  
30  
20  
10  
0
1.2  
1.0  
0.8  
0.6  
0.4  
4
2
1.2  
0.8  
TYPE 52  
POWDERED IRON  
Kool Mµ®  
0.4  
PERMALLOY  
µ = 125  
0.2  
0.01  
0.001  
CORE LOSS IS  
INDEPENDENT OF LOAD  
CURRENT UNTIL LOAD CURRENT FALLS  
LOW ENOUGH FOR CIRCUIT TO GO INTO  
DISCONTINUOUS MODE  
0.12  
0.08  
0.04  
0.02  
3
0
1
2
4
5
0
5
10  
15  
20  
25  
–25  
0
25  
50  
75  
125  
–50  
100  
SWITCH CURRENT (A)  
INDUCTANCE (µH)  
JUNCTION TEMPERATURE (°C)  
1374 G16  
1374 G11  
1374 G01  
U
U
U
PI FU CTIO S  
FB/SENSE: The feedback pin is the input to the error  
amplifier which is referenced to an internal 2.42V source.  
An external resistive divider is used to set the output  
voltage. The fixed voltage (-5) parts have the divider  
included on-chip and the FB pin is used as a SENSE pin,  
connected directly to the 5V output. Three additional  
functions are performed by the FB pin. When the pin  
voltage drops below 1.7V, switch current limit is reduced.  
Below 1.5V the external sync function is disabled. Below  
1V,switchingfrequencyisalsoreduced.SeeFeedbackPin  
Function section in Applications Information for details.  
pins of the 16-lead TSSOP package must be shorted  
together on the PC board.  
GND: The GND pin connection needs consideration for  
tworeasons. First, itactsasthereferencefortheregulated  
output, so load regulation will suffer if the “ground” end of  
the load is not at the same voltage as the GND pin of the  
IC. This condition will occur when load current or other  
currents flow through metal paths between the GND pin  
and the load ground point. Keep the ground path short  
between the GND pin and the load and use a ground plane  
when possible. The second consideration is EMI caused  
by GND pin current spikes. Internal capacitance between  
the VSW pin and the GND pin creates very narrow (<10ns)  
current spikes in the GND pin. If the GND pin is connected  
to system ground with a long metal trace, this trace may  
radiate excess EMI. Keep the path between the input  
bypass and the GND pin short.  
BOOST: The BOOST pin is used to provide a drive voltage,  
higher than the input voltage, to the internal bipolar NPN  
power switch. Without this added voltage, the typical  
switch voltage loss would be about 1.5V. The additional  
boost voltage allows the switch to saturate and voltage  
loss approximates that of a 0.07FET structure. Effi-  
ciency improves from 75% for conventional bipolar de-  
signs to > 89% for these new parts.  
V
SW: The switch pin is the emitter of the on-chip power  
NPN switch. This pin is driven up to the input pin voltage  
during switch on time. Inductor current drives the switch  
pin negative during switch off time. Negative voltage is  
clampedwiththeexternalcatchdiode. Maximumnegative  
switch voltage allowed is 0.8V. Both VSW pins of the  
16-lead TSSOP package must be shorted together on the  
PC board.  
VIN: This is the collector of the on-chip power NPN switch.  
Thispinpowerstheinternalcircuitryandinternalregulator  
whentheBIASpinisnotpresent.AtNPNswitchonandoff,  
high dI/dt edges occur on this pin. Keep the external  
bypass and catch diode close to this pin. All trace induc-  
tance on this path will create a voltage spike at switch off,  
addingtotheVCE voltageacrosstheinternalNPN.BothVIN  
1374fb  
6
LT1374  
U
U
U
PI FU CTIO S  
SYNC: (Excludes T7 package) The sync pin is used to  
synchronize the internal oscillator to an external signal. It  
is directly logic compatible and can be driven with any  
signal between 10% and 90% duty cycle. The synchroniz-  
ing range is equal to initial operating frequency, up to  
1MHz.ThispinreplacesSHDNon-SYNCoptionparts.See  
Synchronizing section in Applications Information for  
details.  
used for frequency compensation, but can do double duty  
as a current clamp or control loop override. This pin sits  
at about 1V for very light loads and 2V at maximum load.  
It can be driven to ground to shut off the regulator, but if  
driven high, current must be limited to 4mA.  
BIAS: (SO-8 and FE16 Packages) The BIAS pin is used to  
improve efficiency when operating at higher input volt-  
ages and light load current. Connecting this pin to the  
regulated output voltage forces most of the internal cir-  
cuitrytodrawitsoperatingcurrentfromtheoutputvoltage  
rather than the input supply. This is a much more efficient  
way of doing business if the input voltage is much higher  
than the output. Minimum output voltage setting for this  
mode of operation is 3.3V. Efficiency improvement at  
VIN = 20V, VOUT = 5V, and IOUT = 25mA is over 10%.  
SHDN: The shutdown pin is used to turn off the regulator  
and to reduce input drain current to a few microamperes.  
Actually, this pin has two separate thresholds, one at  
2.38V to disable switching, and a second at 0.4V to force  
complete micropower shutdown. The 2.38V threshold  
functions as an accurate undervoltage lockout (UVLO).  
This can be used to prevent the regulator from operating  
until the input voltage has reached a predetermined level.  
NC: No Connect. Leave floating or solder to any node.  
VC: The VC pin is the output of the error amplifier and the  
input of the peak switch current comparator. It is normally  
W
BLOCK DIAGRA  
The LT1374 is a constant frequency, current mode buck  
converter. This means that there is an internal clock and  
twofeedbackloopsthatcontrolthedutycycleofthepower  
switch. In addition to the normal error amplifier, there is a  
current sense amplifier that monitors switch current on a  
cycle-by-cycle basis. A switch cycle starts with an oscilla-  
tor pulse which sets the RS flip-flop to turn the switch on.  
When switch current reaches a level set by the inverting  
input of the comparator, the flip-flop is reset and the  
switch turns off. Output voltage control is obtained by  
using the output of the error amplifier to set the switch  
current trip point. This technique means that the error  
amplifier commands current to be delivered to the output  
rather than voltage. A voltage fed system will have low  
phase shift up to the resonant frequency of the inductor  
and output capacitor, then an abrupt 180° shift will occur.  
The current fed system will have 90° phase shift at a much  
lower frequency, but will not have the additional 90° shift  
until well beyond the LC resonant frequency. This makes  
itmucheasiertofrequencycompensatethefeedbackloop  
and also gives much quicker transient response.  
Most of the circuitry of the LT1374 operates from an  
internal 2.9V bias line. The bias regulator normally draws  
power from the regulator input pin, but if the BIAS pin is  
connected to an external voltage higher than 3V, bias  
powerwillbedrawnfromtheexternalsource(typicallythe  
regulated output voltage). This will improve efficiency if  
the BIAS pin voltage is lower than regulator input voltage.  
High switch efficiency is attained by using the BOOST pin  
to provide a voltage to the switch driver which is higher  
thantheinputvoltage,allowingtheswitchtosaturate.This  
boosted voltage is generated with an external capacitor  
and diode. Two comparators are connected to the shut-  
down pin. One has a 2.38V threshold for undervoltage  
lockout and the second has a 0.4V threshold for complete  
shutdown.  
1374fb  
7
LT1374  
W
BLOCK DIAGRA  
0.01Ω  
INPUT  
+
CURRENT  
SENSE  
2.9V BIAS  
REGULATOR  
INTERNAL  
CC  
BIAS*  
AMPLIFIER  
VOLTAGE GAIN = 20  
V
SLOPE COMP  
BOOST  
Σ
0.9V  
500kHz  
OSCILLATOR  
S
R
SYNC  
Q1  
POWER  
SWITCH  
R
DRIVER  
CIRCUITRY  
CURRENT  
COMPARATOR  
S
FLIP-FLOP  
+
SHUTDOWN  
COMPARATOR  
+
V
SW  
0.4V  
FREQUENCY  
SHDN  
SHIFT CIRCUIT  
3.5µA  
FOLDBACK  
CURRENT  
LIMIT  
Q2  
+
CLAMP  
FB  
LOCKOUT  
COMPARATOR  
+
ERROR  
V
C
AMPLIFIER  
2.38V  
2.42V  
g
= 2000µMho  
m
GND  
*BIAS PIN IS AVAILABLE ONLY ON THE S0-8 AND FE16 PACKAGES  
1374 BD  
Figure 1. Block Diagram  
W U U  
U
APPLICATIO S I FOR ATIO  
FEEDBACK PIN FUNCTIONS  
Please read the following if divider resistors are increased  
above the suggested values.  
The feedback (FB) pin on the LT1374 is used to set output  
voltage and provide several overload protection features.  
The first part of this section deals with selecting resistors  
to set output voltage and the remaining part talks about  
foldback frequency and current limiting created by the FB  
pin. Please read both parts before committing to a final  
design. The fixed 5V LT1374-5 has internal divider resis-  
tors and the FB pin is renamed SENSE, connected directly  
to the output.  
R2 V 2.42  
(
)
OUT  
R1=  
2.42  
Table 1  
OUTPUT  
VOLTAGE  
(V)  
R1  
(NEAREST 1%)  
(k  
% ERROR AT OUTPUT  
DUE TO DISCREET 1%  
RESISTOR STEPS  
R2  
(k  
4.99  
4.99  
4.99  
4.99  
4.99  
4.99  
4.99  
4.99  
)
)  
3
3.3  
5
1.21  
1.82  
5.36  
7.32  
11.5  
15.8  
19.6  
26.1  
+0.23  
+0.08  
+0.39  
0.5  
The suggested value for the output divider resistor (see  
Figure 2) from FB to ground (R2) is 5k or less, and a  
formula for R1 is shown below. The output voltage error  
caused by ignoring the input bias current on the FB pin is  
less than 0.25% with R2 = 5k. A table of standard 1%  
values is shown in Table 1 for common output voltages.  
6
8
0.04  
+0.83  
0.62  
+0.52  
10  
12  
15  
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More Than Just Voltage Feedback  
foldback operation. Again, it is nearly transparent to the  
userundernormalloadconditions.Theonlyloadsthatmay  
be affected are current source loads which maintain full  
loadcurrentwithoutputvoltagelessthan50%offinalvalue.  
In these rare situations the feedback pin can be clamped  
above 1.5V with an external diode to defeat foldback cur-  
rent limit. Caution: clamping the feedback pin means that  
frequency shifting will also be defeated, so a combination  
of high input voltage and dead shorted output may cause  
the LT1374 to lose control of current limit.  
The feedback pin is used for more than just output voltage  
sensing. It also reduces switching frequency and current  
limit when output voltage is very low (see the Frequency  
Foldback graph in Typical Performance Characteristics).  
ThisisdonetocontrolpowerdissipationinboththeICand  
in the external diode and inductor during short-circuit  
conditions. A shorted output requires the switching regu-  
lator to operate at very low duty cycles, and the average  
current through the diode and inductor is equal to the  
short-circuitcurrentlimitoftheswitch(typically6Aforthe  
LT1374, foldingbacktolessthan3A). Minimumswitchon  
time limitations would prevent the switcher from attaining  
a sufficiently low duty cycle if switching frequency were  
maintained at 500kHz, so frequency is reduced by about  
5:1 when the feedback pin voltage drops below 1V (see  
FrequencyFoldbackgraph). Thisdoesnotaffectoperation  
with normal load conditions; one simply sees a gear shift  
in switching frequency during start-up as the output  
voltage rises.  
The internal circuitry which forces reduced switching  
frequency also causes current to flow out of the feedback  
pin when output voltage is low. The equivalent circuitry is  
shown in Figure 2. Q1 is completely off during normal  
operation. If the FB pin falls below 1V, Q1 begins to  
conduct current and reduces frequency at the rate of  
approximately 5kHz/µA. To ensure adequate frequency  
foldback (under worst-case short-circuit conditions), the  
external divider Thevinin resistance must be low enough  
to pull 150µA out of the FB pin with 0.6V on the pin (RDIV  
4k). The net result is that reductions in frequency and  
current limit are affected by output voltage divider imped-  
ance. Although divider impedance is not critical, caution  
should be used if resistors are increased beyond the  
suggested values and short-circuit conditions will occur  
with high input voltage. High frequency pickup will  
increase and the protection accorded by frequency and  
current foldback will decrease.  
In addition to lower switching frequency, the LT1374 also  
operates at lower switch current limit when the feedback  
pin voltage drops below 1.7V. Q2 in Figure 2 performs this  
function by clamping the VC pin to a voltage less than its  
normal 2.1V upper clamp level. This foldback current limit  
greatly reduces power dissipation in the IC, diode and  
inductorduringshort-circuitconditions.Externalsynchro-  
nization is also disabled to prevent interference with  
LT1374  
V
SW  
TO FREQUENCY  
OUTPUT  
5V  
SHIFTING  
1.6V  
Q1  
ERROR  
AMPLIFIER  
2.4V  
+
R1  
R3  
1k  
R4  
1k  
FB  
+
R5  
5k  
Q2  
R2  
5k  
TO SYNC CIRCUIT  
V
C
GND  
1374 F02  
Figure 2. Frequency and Current Limit Foldback  
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MAXIMUM OUTPUT LOAD CURRENT  
Note that there is less load current available at the higher  
input voltage because inductor ripple current increases.  
This is not always the case. Certain combinations of  
inductor value and input voltage range may yield lower  
available load current at the lowest input voltage due to  
reduced peak switch current at high duty cycles. If load  
current is close to the maximum available, please check  
maximum available current at both input voltage  
extremes. To calculate actual peak switch current with a  
given set of conditions, use:  
Maximum load current for a buck converter is limited by  
the maximum switch current rating (IP) of the LT1374.  
This current rating is 4.5A up to 50% duty cycle (DC),  
decreasing to 3.7A at 80% duty cycle. This is shown  
graphically in Typical Performance Characteristics and as  
shown in the formula below:  
IP = 4.5A for DC 50%  
IP = 3.21 + 5.95(DC) – 6.75(DC)2 for 50% < DC < 90%  
DC = Duty cycle = VOUT/VIN  
VOUT V V  
(
)
IN  
OUT  
Example: with VOUT = 5V, VIN = 8V; DC = 5/8 = 0.625, and;  
ISW(MAX) = 3.21 + 5.95(0.625) – 6.75(0.625)2 = 4.3A  
ISW PEAK =IOUT  
+
(
)
2 L f V  
( )( )( )  
IN  
For lighter loads where discontinuous operation can be  
used, maximum load current is equal to:  
Current rating decreases with duty cycle because the  
LT1374hasinternalslopecompensationtopreventcurrent  
mode subharmonic switching. For more details, read Ap-  
plicationNote19.TheLT1374isalittleunusualinthisregard  
because it has nonlinear slope compensation which gives  
better compensation with less reduction in current limit.  
2
I
f L V  
IN  
( ) ( )( )(  
)
P
IOUT(MAX)  
=
Discontinuous mode 2 V  
V V  
(
)(  
)
OUT  
IN  
OUT  
Example: with L = 1.2µH, VOUT = 5V, and VIN(MAX) = 15V,  
Maximum load current would be equal to maximum  
switch current for an infinitely large inductor, but with  
finite inductor size, maximum load current is reduced by  
one-half peak-to-peak inductor current. The following  
formula assumes continuous mode operation, implying  
that the term on the right is less than one-half of IP.  
2
4.5 500 103 1.2 106 15  
(
)
( )  
IOUT MAX  
=
= 1.82A  
(
)
2 5 15 5  
( )(  
)
The main reason for using such a tiny inductor is that it is  
physically very small, but keep in mind that peak-to-peak  
inductorcurrentwillbeveryhigh. Thiswillincreaseoutput  
ripplevoltage.Iftheoutputcapacitorhastobemadelarger  
to reduce ripple voltage, the overall circuit could actually  
wind up larger.  
V
V V  
IN OUT  
(
OUT)(  
)
IOUT(MAX)  
=
IP −  
Continuous Mode  
2 L f V  
( )( )( )  
IN  
For the conditions above and L = 3.3µH,  
5 8 5  
( )(  
)
CHOOSING THE INDUCTOR AND OUTPUT CAPACITOR  
IOUT MAX) = 4.3 −  
(
2 3.3 106 500103  
8
( )  
For most applications the output inductor will fall in the  
range of 3µH to 20µH. Lower values are chosen to reduce  
physical size of the inductor. Higher values allow more  
output current because they reduce peak current seen by  
the LT1374 switch, which has a 4.5A limit. Higher values  
also reduce output ripple voltage, and reduce core loss.  
GraphsintheTypicalPerformanceCharacteristicssection  
show maximum output load current versus inductor size  
andinputvoltage. Asecondgraphshowscorelossversus  
=4.3 0.57= 3.73A  
AtVIN =15V, dutycycleis33%, soIP isjustequaltoafixed  
4.5A, and IOUT(MAX) is equal to:  
5 15 5  
( )(  
)
4.5 −  
2 3.3 106 500103 15  
( )  
= 4.5 1= 3.5A  
inductor size for various core materials.  
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core next to a magnetic storage media, for instance!  
Thisisatoughdecisionbecausetherodsorbarrelsare  
temptingly cheap and small and there are no helpful  
guidelines to calculate when the magnetic field radia-  
tion will be a problem.  
When choosing an inductor you might have to consider  
maximum load current, core and copper losses, allowable  
component height, output voltage ripple, EMI, fault cur-  
rent in the inductor, saturation, and of course, cost. The  
following procedure is suggested as a way of handling  
thesesomewhatcomplicatedandconflictingrequirements.  
4. Start shopping for an inductor (see representative  
surface mount units in Table 2) which meets the  
requirements of core shape, peak current (to avoid  
1. Choose a value in microhenries from the graphs of  
maximumloadcurrentandcoreloss.Choosingasmall  
inductor may result in discontinuous mode operation  
at lighter loads, but the LT1374 is designed to work  
well in either mode. Keep in mind that lower core loss  
means higher cost, at least for closed core geometries  
like toroids. The core loss graphs show both absolute  
lossandpercentlossfora5Woutput,soactualpercent  
losses must be calculated for each situation.  
Table 2  
SERIES  
RESIS-  
CORE  
MATER- HEIGHT  
IAL  
VENDOR/  
PART NO.  
VALUE  
DC  
CORE  
(
µ
H) (Amps) TYPE TANCE(  
)
(mm)  
Coiltronics  
CTX2-1  
2
4.1  
4.4  
3.5  
3.4  
4.6  
3.3  
Tor  
Tor  
Tor  
Tor  
Tor  
Tor  
0.011  
KMµ  
KMµ  
KMµ  
52  
4.2  
6.4  
6.4  
4.2  
4.8  
6.4  
CTX5-4  
5
8
2
2
5
0.019  
0.020  
0.014  
0.012  
0.027  
CTX8-4  
Assume that the average inductor current is equal to  
load current and decide whether or not the inductor  
must withstand continuous fault conditions. If maxi-  
mum load current is 0.5A, for instance, a 0.5A inductor  
may not survive a continuous 4.5A overload condition.  
Dead shorts will actually be more gentle on the induc-  
tor because the LT1374 has foldback current limiting.  
CTX2-1P  
CTX2-3P  
52  
CTX5-4P  
52  
Sumida  
CDRH125  
CDRH125  
CDRH125  
CDRH125  
Coilcraft  
10  
12  
15  
18  
4.0  
3.5  
3.3  
3.0  
SC  
SC  
SC  
SC  
0.025  
0.027  
0.030  
0.034  
Fer  
Fer  
Fer  
Fer  
6
6
6
6
2. Calculate peak inductor current at full load current to  
ensure that the inductor will not saturate. Peak current  
can be significantly higher than output current, espe-  
cially with smaller inductors and lighter loads, so don’t  
omit this step. Powdered iron cores are forgiving  
because they saturate softly, whereas ferrite cores  
saturate abruptly. Other core materials fall somewhere  
in between. The following formula assumes continu-  
ous mode of operation, but it errs only slightly on the  
high side for discontinuous mode, so it can be used for  
all conditions.  
DT3316-222  
DT3316-332  
DT3316-472  
Pulse  
2.2  
3.3  
4.7  
5
5
3
SC  
SC  
SC  
0.035  
0.040  
0.045  
Fer  
Fer  
Fer  
5.1  
5.1  
5.1  
PE-53650  
PE-53651  
PE-53652  
PE-53653  
Dale  
4
5
4.8  
5.4  
5.5  
5.1  
Tor  
Tor  
Tor  
Tor  
0.017  
0.018  
0.022  
0.032  
Fer  
Fer  
Fer  
Fer  
9.1  
9.1  
10  
9
16  
10  
VOUT V V  
(
)
IN  
OUT  
IHSM-4825  
IHSM-4825  
IHSM-5832  
IHSM-5832  
IHSM-7832  
Tor = Toroid  
2.7  
4.7  
10  
5.1  
4.0  
4.3  
3.5  
3.8  
Open  
Open  
Open  
Open  
Open  
0.034  
0.047  
0.053  
0.078  
0.054  
Fer  
Fer  
Fer  
Fer  
Fer  
5.6  
5.6  
7.1  
7.1  
7.1  
IPEAK =IOUT +  
2 f L V  
( )( )( )  
IN  
VIN = Maximum input voltage  
f = Switching frequency, 500kHz  
15  
22  
3. Decide if the design can tolerate an “open” core geom-  
etry like a rod or barrel, with high magnetic field  
radiation, orwhetheritneedsaclosedcorelikeatoroid  
to prevent EMI problems. One would not want an open  
SC = Semi-closed geometry  
Fer = Ferrite core material  
52 = Type 52 powdered iron core material  
KMµ = Kool Mµ  
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saturation),averagecurrent(tolimitheating),andfault  
current(iftheinductorgetstoohot, wireinsulationwill  
melt and cause turn-to-turn shorts). Keep in mind that  
allgoodthingslikehighefficiency,lowprofile,andhigh  
temperature operation will increase cost, sometimes  
dramatically. Get a quote on the cheapest unit first to  
calibrate yourself on price, then ask for what you really  
want.  
Many engineers have heard that solid tantalum capacitors  
are prone to failure if they undergo high surge currents.  
This is historically true, and type TPS capacitors are  
speciallytestedforsurgecapability,butsurgeruggedness  
is not a critical issue with the output capacitor. Solid  
tantalum capacitors fail during very high turn-on surges,  
which do not occur at the output of regulators. High  
discharge surges, such as when the regulator output is  
dead shorted, do not harm the capacitors.  
5. After making an initial choice, consider the secondary  
things like output voltage ripple, second sourcing, etc.  
Use the experts in the Linear Technology’s applica-  
tions department if you feel uncertain about the final  
choice. They have experience with a wide range of  
inductor types and can tell you about the latest devel-  
opments in low profile, surface mounting, etc.  
Unlike the input capacitor, RMS ripple current in the  
output capacitor is normally low enough that ripple cur-  
rent rating is not an issue. The current waveform is  
triangular with a typical value of 200mARMS. The formula  
to calculate this is:  
Output Capacitor Ripple Current (RMS):  
Output Capacitor  
0.29 V  
V V  
IN OUT  
(
OUT)(  
)
The output capacitor is normally chosen by its Effective  
Series Resistance (ESR), because this is what determines  
output ripple voltage. At 500kHz, any polarized capacitor  
is essentially resistive. To get low ESR takes volume, so  
physically smaller capacitors have high ESR. The ESR  
range for typical LT1374 applications is 0.05to 0.2. A  
typical output capacitor is an AVX type TPS, 100µF at 10V,  
with a guaranteed ESR less than 0.1. This is a “D” size  
surface mount solid tantalum capacitor. TPS capacitors  
are specially constructed and tested for low ESR, so they  
give the lowest ESR for a given volume. The value in  
microfarads is not particularly critical, and values from  
22µF to greater than 500µF work well, but you cannot  
cheat mother nature on ESR. If you find a tiny 22µF solid  
tantalumcapacitor, itwillhavehighESR, andoutputripple  
voltage will be terrible. Table 3 shows some typical solid  
tantalum surface mount capacitors.  
IRIPPLE RMS  
=
(
)
L f V  
( )( )( )  
IN  
Ceramic Capacitors  
Higher value, lower cost ceramic capacitors are now  
becomingavailableinsmallercasesizes.Thesearetempt-  
ing for switching regulator use because of their very low  
ESR. Unfortunately, the ESR is so low that it can cause  
loop stability problems. Solid tantalum capacitor’s ESR  
generatesaloopzeroat5kHzto50kHzthatisinstrumen-  
tal in giving acceptable loop phase margin. Ceramic  
capacitors remain capacitive to beyond 300kHz and usu-  
allyresonatewiththeirESLbeforeESRbecomeseffective.  
They are appropriate for input bypassing because of their  
highripplecurrentratingsandtoleranceofturn-onsurges.  
Linear Technology plans to issue a design note on the use  
of ceramic capacitors in the near future.  
Table 3. Surface Mount Solid Tantalum Capacitor ESR  
and Ripple Current  
OUTPUT RIPPLE VOLTAGE  
E Case Size  
ESR (Max.,  
)
Ripple Current (A)  
0.7 to 1.1  
0.4  
AVX TPS, Sprague 593D  
AVX TAJ  
0.1 to 0.3  
0.7 to 0.9  
Figure 3 shows a typical output ripple voltage waveform  
for the LT1374. Ripple voltage is determined by the high  
frequency impedance of the output capacitor, and ripple  
current through the inductor. Peak-to-peak ripple current  
through the inductor into the output capacitor is:  
D Case Size  
AVX TPS, Sprague 593D  
C Case Size  
0.1 to 0.3  
0.2 (typ)  
0.7 to 1.1  
0.5 (typ)  
AVX TPS  
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CATCH DIODE  
V
V V  
IN OUT  
(
OUT)(  
)
IP-P  
=
The suggested catch diode (D1) is a 1N5821 Schottky, or  
its Motorola equivalent, MBR330. It is rated at 3A average  
forward current and 30V reverse voltage. Typical forward  
voltage is 0.5V at 3A. The diode conducts current only  
during switch off time. Peak reverse voltage is equal to  
regulatorinputvoltage.Averageforwardcurrentinnormal  
operation can be calculated from:  
V
L f  
( )( )( )  
IN  
For high frequency switchers, the sum of ripple current  
slew rates may also be relevant and can be calculated  
from:  
dI  
dt  
V
IN  
L
Σ
=
IOUT V V  
(
)
IN  
OUT  
ID
(
AVG  
=
Peak-to-peak output ripple voltage is the sum of a triwave  
created by peak-to-peak ripple current times ESR, and a  
square wave created by parasitic inductance (ESL) and  
ripple current slew rate. Capacitive reactance is assumed  
to be small compared to ESR or ESL.  
)
V
IN  
This formula will not yield values higher than 3A with  
maximumloadcurrentof4.25Aunlesstheratioofinputto  
output voltage exceeds 3.4:1. The only reason to consider  
a larger diode is the worst-case condition of a high input  
voltageandoverloaded(notshorted)output. Undershort-  
circuit conditions, foldback current limit will reduce diode  
current to less than 2.6A, but if the output is overloaded  
anddoesnotfalltolessthan1/3ofnominaloutputvoltage,  
foldback will not take effect. With the overloaded condi-  
tion, output current will increase to a typical value of 5.7A,  
determined by peak switch current limit of 6A. With  
VIN = 15V, VOUT = 4V (5V overloaded) and IOUT = 5.7A:  
dI  
dt  
VRIPPLE = I  
ESR + ESL Σ  
(
P-P)(  
) (  
)
Example: withVIN =10V,VOUT =5V,L=10µH,ESR=0.1,  
ESL = 10nH:  
5 10 5  
( )(  
)
IP-P  
=
= 0.5A  
10 10 106 500 103  
( )  
5.7 15 4  
(
)
dI  
dt  
10  
Σ
=
= 106  
I
=
= 4.18A  
D AVG  
(
)
10 106  
15  
VRIPPLE = 0.5A 0.1 + 10 109 106  
This is safe for short periods of time, but it would be  
prudent to check with the diode manufacturer if continu-  
ous operation under these conditions must be tolerated.  
(
)(  
)
= 0.05 + 0.01= 60mVP-P  
BOOST PIN CONSIDERATIONS  
Formostapplications, theboostcomponentsarea0.27µF  
capacitor and a FMMD914 diode. The anode is connected  
to the regulated output voltage and this generates a  
voltage across the boost capacitor nearly identical to the  
regulated output. In certain applications, the anode may  
instead be connected to the unregulated input voltage.  
This could be necessary if the regulated output voltage is  
very low (< 3V) or if the input voltage is less than 5V.  
Efficiency is not affected by the capacitor value, but the  
capacitor should have an ESR of less than 1to ensure  
1374fb  
V
OUT AT  
IOUT = 1A  
20mV/DIV  
0.5A/DIV  
V
OUT AT  
IOUT = 50mA  
INDUCTOR  
CURRENT  
AT IOUT = 1A  
INDUCTOR  
CURRENT  
AT IOUT = 50mA  
0.5µs/DIV  
1374 F03  
Figure 3. LT1374 Ripple Voltage Waveform  
13  
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that it can be recharged fully under the worst-case condi-  
tion of minimum input voltage. Almost any type of film or  
ceramic capacitor will work fine.  
I
/50 VOUT / V  
(
)(  
)
OUT  
IN  
CMIN  
=
f V 3V  
( )(  
)
OUT  
WARNING! Peak voltage on the BOOST pin is the sum of  
unregulated input voltage plus the voltage across the  
boost capacitor. This normally means that peak BOOST  
pin voltage is equal to input voltage plus output voltage,  
but when the boost diode is connected to the regulator  
input, peak BOOST pin voltage is equal to twice the input  
voltage. Be sure that BOOST pin voltage does not exceed  
its maximum rating.  
f = Switching frequency  
VOUT = Regulated output voltage  
VIN = Minimum input voltage  
This formula can yield capacitor values substantially less  
than 0.27µF, but it should be used with caution since it  
does not take into account secondary factors such as  
capacitor series resistance, capacitance shift with tem-  
perature and output overload.  
For nearly all applications, a 0.27µF boost capacitor works  
just fine, but for the curious, more details are provided  
here. The size of the boost capacitor is determined by  
switch drive current requirements. During switch on time,  
draincurrentonthecapacitorisapproximatelyIOUT/50.At  
peakloadcurrentof4.25A,thisgivesatotaldrainof85mA.  
Capacitor ripple voltage is equal to the product of on time  
and drain current divided by capacitor value;  
V = (tON)(85mA/C). To keep capacitor ripple voltage to  
less than 0.6V (a slightly arbitrary number) at the worst-  
case condition of tON = 1.8µs, the capacitor needs to be  
0.27µF. Boost capacitor ripple voltage is not a critical  
parameter, but if the minimum voltage across the capaci-  
tor drops to less than 3V, the power switch may not  
saturate fully and efficiency will drop. An approximate  
formula for absolute minimum capacitor value is:  
SHUTDOWN FUNCTION AND  
UNDERVOLTAGE LOCKOUT  
Figure 4 shows how to add undervoltage lockout (UVLO)  
to the LT1374. Typically, UVLO is used in situations where  
the input supply is current limited, or has a relatively high  
source resistance. A switching regulator draws constant  
power from the source, so source current increases as  
source voltage drops. This looks like a negative resistance  
loadtothesourceandcancausethesourcetocurrentlimit  
or latch low under low source voltage conditions. UVLO  
prevents the regulator from operating at source voltages  
where these problems might occur.  
R
FB  
LT1374  
IN  
OUTPUT  
V
SW  
INPUT  
2.38V  
+
STANDBY  
R
HI  
3.5µA  
+
SHDN  
+
TOTAL  
SHUTDOWN  
R
LO  
C1  
0.4V  
GND  
1374 F04  
Figure 4. Undervoltage Lockout  
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input rises back to 13.5V. V is therefore 1.5V and  
Threshold voltage for lockout is about 2.38V, slightly less  
than the internal 2.42V reference voltage. A 3.5µA bias  
current flows out of the pin at threshold. This internally  
generated current is used to force a default high state on  
the shutdown pin if the pin is left open. When low shut-  
down current is not an issue, the error due to this current  
can be minimized by making RLO 10k or less. If shutdown  
currentisanissue, RLO canberaisedto100k, buttheerror  
due to initial bias current and changes with temperature  
should be considered.  
VIN = 12V. Let RLO = 25k.  
25k 12 2.38 1.5/5 +1 + 1.5  
(
)
)
[
]
RHI =  
2.38 25k 3.5µA  
(
25k 10.41  
(
)
=
= 114k  
2.29  
R =114k 5/1.5 = 380k  
(
)
FB  
R = 10k to 100k 25k suggested  
(
)
LO  
SWITCH NODE CONSIDERATIONS  
RLO V 2.38V  
(
)
IN  
RHI =  
For maximum efficiency, switch rise and fall times are  
made as short as possible. To prevent radiation and high  
frequency resonance problems, proper layout of the com-  
ponents connected to the switch node is essential. B field  
(magnetic) radiation is minimized by keeping catch diode,  
switch pin, and input bypass capacitor leads as short as  
possible. E field radiation is kept low by minimizing the  
length and area of all traces connected to the switch pin  
and BOOST pin. A ground plane should always be used  
under the switcher circuitry to prevent interplane cou-  
pling. A suggested layout for the critical components is  
shown in Figure 5. Note that the feedback resistors and  
compensation components are kept as far as possible  
from the switch node. Also note that the high current  
groundpathofthecatchdiodeandinputcapacitorarekept  
very short and separate from the analog ground line.  
2.38V RLO 3.5µA  
(
)
VIN = Minimum input voltage  
Keep the connections from the resistors to the shutdown  
pin short and make sure that interplane or surface capaci-  
tance to the switching nodes are minimized. If high  
resistor values are used, the shutdown pin should be  
bypassed with a 1000pF capacitor to prevent coupling  
problems from the switch node. If hysteresis is desired in  
the undervoltage lockout point, a resistor RFB can be  
added to the output node. Resistor values can be calcu-  
lated from:  
RLO V 2.38 V/V +1 + ∆V  
(
)
IN  
OUT  
[
]
RHI =  
2.38 R2 3.5µA  
(
)
Thehighspeedswitchingcurrentpathisshownschemati-  
cally in Figure 6. Minimum lead length in this path is  
essential to ensure clean switching and low EMI. The path  
including the switch, catch diode, and input capacitor is  
the only one containing nanosecond rise and fall times. If  
you follow this path on the PC layout, you will see that it is  
irreducibly short. If you move the diode or input capacitor  
away from the LT1374, get your resumé in order. The  
other paths contain only some combination of DC and  
500kHz triwave, so are much less critical.  
R = R  
V
/V  
(
HI)(  
)
FB  
OUT  
25k suggested for RLO  
VIN = Input voltage at which switching stops as input  
voltage descends to trip level  
V = Hysteresis in input voltage level  
Example: output voltage is 5V, switching is to stop if input  
voltage drops below 12V and should not restart unless  
1374fb  
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APPLICATIONS INFORMATION  
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CONNECT TO  
GROUND PLANE  
MINIMIZE LT1374, C3, D1 LOOP  
V
IN  
C3  
D1  
C5  
GND  
C6  
V
OUT  
1
TAKE OUTPUT  
DIRECTLY FROM  
END OF OUTPUT  
CAPACITOR  
GND  
L1  
U1  
C1  
R3  
R2  
D2  
CONNECT TO  
GROUND PLANE  
PLACE FEEDTHROUGHS  
AROUND GND PIN FOR GOOD  
THERMAL CONDUCTIVITY  
C4  
KELVIN SENSE  
KEEP FB AND V COMPONENTS  
C
AWAY FROM HIGH FREQUENCY,  
HIGH CURRENT COMPONENTS  
V
OUT  
13745 F05a  
Figure 5a. Suggested Layout (Topside Only Shown) SO-8  
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SOLDER EXPOSED PAD AND  
USE FEEDTHROUGHS FOR  
BETTER THERMAL CONDUCTIVITY  
KEEP FB AND V  
C
COMPONENTS AWAY  
FROM HIGH FREQUENCY,  
HIGH CURRENT  
GND  
C3  
V
IN  
COMPONENTS  
C4 C2 R3  
KELVIN  
SENSE  
OUTPUT  
D2  
R2 R1 C1  
V
OUT  
D1  
C1  
1374 F05b  
Figure 5b. Suggested Layout (Topside Only Shown) TSSOP  
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APPLICATIONS INFORMATION  
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MINIMIZE LT1374 C3, D1 LOOP  
CONNECT TO GND PLANE  
C3  
D1  
V
OUT  
V
IN  
TAKE OUTPUT  
DIRECTLY FROM  
END OF OUTPUT  
CAPACITOR  
L1  
PLACE FEEDTHROUGHS  
AROUND GND TAB,  
C3, D1 FOR GOOD  
THERMAL  
D2  
V
OUT  
C4  
R2  
CONDUCTIVITY  
C5  
C6  
C
C2  
KELVIN SENSE  
V
OUT  
C
C
7
6
5
4
3 2 1  
R3  
U1  
R
C
TAB IS GND  
GND  
1374 F05c  
KEEP FB AND V COMPONENTS  
C
AWAY FROM ANY HIGH FREQUENCY,  
HIGH CURRENT CMPONENTS OR PATHS  
Figure 5c. Suggested Layout (Topside Only Shown) DD  
SWITCH NODE  
L1  
5V  
HIGH  
FREQUENCY  
CIRCULATING  
PATH  
V
IN  
LOAD  
1374 F06  
Figure 6. High Speed Switching Path  
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PARASITIC RESONANCE  
Resonance or “ringing” may sometimes be seen on the  
switch node (see Figure 7). Very high frequency ringing  
following switch rise time is caused by switch/diode/input  
capacitor lead inductance and diode capacitance. Schot-  
tky diodes have very high “Q” junction capacitance that  
can ring for many cycles when excited at high frequency.  
Iftotalleadlengthfortheinputcapacitor, diodeandswitch  
path is 1 inch, the inductance will be approximately 25nH.  
At switch off, this will produce a spike across the NPN  
output device in addition to the input voltage. At higher  
currents this spike can be in the order of 10V to 20V or  
higher with a poor layout, potentially exceeding the abso-  
lute max switch voltage. The path around switch, catch  
diode and input capacitor must be kept as short as  
possibletoensurereliableoperation.Whenlookingatthis,  
a >100MHz oscilloscope must be used, and waveforms  
should be observed on the leads of the package. This  
switch off spike will also cause the SW node to go below  
ground. The LT1374 has special circuitry inside which  
mitigates this problem, but negative voltages over 1V  
lasting longer than 10ns should be avoided. Note that  
100MHz oscilloscopes are barely fast enough to see the  
details of the falling edge overshoot in Figure 7.  
RISE AND FALL  
WAVEFORMS ARE  
SUPERIMPOSED  
(PULSE WIDTH IS  
NOT 120ns)  
5V/DIV  
20ns/DIV  
1374 F07  
Figure 7. Switch Node Resonance  
5V/DIV  
SWITCH NODE  
VOLTAGE  
INDUCTOR  
CURRENT  
100mA/DIV  
20ns/DIV  
1375/76 F11  
0.5µs/DIV  
1374 F08  
Figure 8. Discontinuous Mode Ringing  
current fed back into the input supply. The capacitor also  
forces switching current to flow in a tight local loop,  
minimizing EMI.  
A second, much lower frequency ringing is seen during  
switch off time if load current is low enough to allow the  
inductor current to fall to zero during part of the switch off  
time (see Figure 8). Switch and diode capacitance reso-  
nate with the inductor to form damped ringing at 1MHz to  
10 MHz. This ringing is not harmful to the regulator and it  
hasnotbeenshowntocontributesignificantlytoEMI. Any  
attempt to damp it with a resistive snubber will degrade  
efficiency.  
Do not cheat on the ripple current rating of the Input  
bypass capacitor, but also don’t get hung up on the value  
in microfarads. The input capacitor is intended to absorb  
all the switching current ripple, which can have an RMS  
value as high as one half of load current. Ripple current  
ratings on the capacitor must be observed to ensure  
reliable operation. In many cases it is necessary to parallel  
two capacitors to obtain the required ripple rating. Both  
capacitors must be of the same value and manufacturer to  
guaranteepowersharing. Theactualvalueofthecapacitor  
in microfarads is not particularly important because at  
500kHz, any value above 5µF is essentially resistive. RMS  
ripple current rating is the critical parameter. Actual RMS  
current can be calculated from:  
INPUT BYPASSING AND VOLTAGE RANGE  
Input Bypass Capacitor  
Step-down converters draw current from the input supply  
in pulses. The average height of these pulses is equal to  
load current, and the duty cycle is equal to VOUT/VIN. Rise  
and fall time of the current is very fast. A local bypass  
capacitor across the input supply is necessary to ensure  
proper operation of the regulator and minimize the ripple  
2
IRIPPLE RMS =IOUT VOUT V V  
/V  
IN  
(
)
IN  
OUT  
(
)
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The term inside the radical has a maximum value of 0.5  
when input voltage is twice output, and stays near 0.5 for  
a relatively wide range of input voltages. It is common  
practice therefore to simply use the worst-case value and  
assumethatRMSripplecurrentisonehalfofloadcurrent.  
At maximum output current of 4.5A for the LT1374, the  
input bypass capacitor should be rated at 2.25A ripple  
current. Note however, that there are many secondary  
considerations in choosing the final ripple current rating.  
These include ambient temperature, average versus peak  
load current, equipment operating schedule, and required  
product lifetime. For more details, see Application Notes  
19 and 46, and Design Note 95.  
Larger capacitors may be necessary when the input volt-  
age is very close to the minimum specified on the data  
sheet. Small voltage dips during switch on time are not  
normallyaproblem, butatverylowinputvoltagetheymay  
cause erratic operation because the input voltage drops  
below the minimum specification. Problems can also  
occur if the input-to-output voltage differential is near  
minimum. The amplitude of these dips is normally a  
function of capacitor ESR and ESL because the capacitive  
reactance is small compared to these terms. ESR tends to  
be the dominate term and is inversely related to physical  
capacitor size within a given capacitor type.  
SYNCHRONIZING (Available as -SYNC Option)  
Input Capacitor Type  
The LT1374-SYNC has the SHDN pin replaced with a  
SYNC pin, which is used to synchronize the internal  
oscillator to an external signal. The SYNC input must pass  
from a logic level low, through the maximum synchroni-  
zation threshold with a duty cycle between 10% and 90%.  
The input can be driven directly from a logic level output.  
The synchronizing range is equal to initial operating fre-  
quency up to 1MHz. This means that minimum practical  
sync frequency is equal to the worst-case high self-  
oscillating frequency (550kHz), not the typical operating  
frequency of 500kHz. Caution should be used when syn-  
chronizing above 700kHz because at higher sync frequen-  
cies the amplitude of the internal slope compensation  
used to prevent subharmonic switching is reduced. This  
type of subharmonic switching only occurs at input volt-  
ages less than twice output voltage. Higher inductor  
values will tend to eliminate this problem. See Frequency  
Compensation section for a discussion of an entirely  
different cause of subharmonic switching before assum-  
ing that the cause is insufficient slope compensation.  
ApplicationNote19hasmoredetailsonthetheoryofslope  
compensation.  
Some caution must be used when selecting the type of  
capacitor used at the input to regulators. Aluminum  
electrolytics are lowest cost, but are physically large to  
achieve adequate ripple current rating, and size con-  
straints (especially height), may preclude their use.  
Ceramic capacitors are now available in larger values, and  
their high ripple current and voltage rating make them  
ideal for input bypassing. Cost is fairly high and footprint  
may also be somewhat large. Solid tantalum capacitors  
would be a good choice, except that they have a history of  
occasionalspectacularfailureswhentheyaresubjectedto  
large current surges during power-up. The capacitors can  
short and then burn with a brilliant white light and lots of  
nasty smoke. This phenomenon occurs in only a small  
percentage of units, but it has led some OEM companies  
to forbid their use in high surge applications. The input  
bypass capacitor of regulators can see these high surges  
when a battery or high capacitance source is connected.  
Several manufacturers have developed a line of solid  
tantalum capacitors specially tested for surge capability  
(AVX TPS series for instance, see Table 3), but even these  
units may fail if the input voltage surge approaches the  
maximum voltage rating of the capacitor. AVX recom-  
mends derating capacitor voltage by 2:1 for high surge  
applications. The highest voltage rating is 50V, so 25V  
may be a practical upper limit when using solid tantalum  
capacitors for input bypassing.  
At power-up, when VC is being clamped by the FB pin (see  
Figure2,Q2),thesyncfunctionisdisabled.Thisallowsthe  
frequency foldback to operate in the shorted output con-  
dition. During normal operation, switching frequency is  
controlledbytheinternaloscillatoruntiltheFBpinreaches  
1.5V, after which the SYNC pin becomes operational. If no  
synchronization is required, this pin should be connected  
to ground.  
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THERMAL CALCULATIONS  
Thermal resistance for LT1374 package is influenced by  
the presence of internal or backside planes. With a full  
plane under the 16-lead TSSOP package, thermal resis-  
tance will be about 40°C/W. To calculate die temperature,  
use the proper thermal resistance number for the desired  
package and add in worst-case ambient temperature:  
Power dissipation in the LT1374 chip comes from four  
sources: switch DC loss, switch AC loss, boost circuit  
current,andinputquiescentcurrent.Thefollowingformu-  
las show how to calculate each of these losses. These  
formulas assume continuous mode operation, so they  
should not be used for calculating efficiency at light load  
currents.  
TJ = TA + θJA (PTOT  
)
WiththeTSSOP16package(θJA =40°C/W), atanambient  
temperature of 50°C,  
Switch loss:  
TJ = 50 + 40 (0.87) = 85°C  
2
R
I
V
OUT  
(
) (  
)
SW OUT  
For the DD package with a good copper plane under the  
device, thermal resistance will be about 30°C/W. For the  
conditions above:  
P
=
+ 24ns I  
V
f
(
)( )( )  
SW  
OUT IN  
V
IN  
Boost current loss:  
TJ = 50 + 30 (0.87) = 76°C  
2
V
I
/50  
(
)
OUT OUT  
Die temperature is highest at low input voltage, so use  
lowest continuous input operating voltage for thermal  
calculations.  
P
=
BOOST  
V
IN  
Quiescent current loss:  
FREQUENCY COMPENSATION  
2
VOUT 0.002  
(
)
Loop frequency compensation of switching regulators  
can be a rather complicated problem because the reactive  
components used to achieve high efficiency also intro-  
duce multiple poles into the feedback loop. The inductor  
and output capacitor on a conventional step-down con-  
verter actually form a resonant tank circuit that can exhibit  
peaking and a rapid 180° phase shift at the resonant  
frequency. Bycontrast, theLT1374usesacurrentmode”  
architecture to help alleviate phase shift created by the  
inductor. The basic connections are shown in Figure 9.  
Figure 10 shows a Bode plot of the phase and gain of the  
power section of the LT1374, measured from the VC pin to  
the output. Gain is set by the 5.3A/V transconductance of  
the LT1374 power section and the effective complex  
impedance from output to ground. Gain rolls off smoothly  
above the 600Hz pole frequency set by the 100µF output  
capacitor. Phase drop is limited to about 70°. Phase  
recoversandgainlevelsoffatthezerofrequency(16kHz)  
set by capacitor ESR (0.1).  
P =V 0.001 + V  
0.005 +  
(
)
(
)
Q
IN  
OUT  
V
IN  
RSW = Switch resistance (0.07)  
24ns = Equivalent switch current/voltage overlap time  
f = Switch frequency  
Example: with VIN = 10V, VOUT = 5V and IOUT = 3A:  
2
0.07 3  
5
(
)( ) ( )  
PSW  
=
+ 24 109 3 10 500103  
( )( )  
10  
= 0.32 + 0.36 = 0.68W  
2
5
3/50  
( ) (  
)
PBOOST  
=
= 0.15W  
10  
2
5
0.002  
( ) (  
)
P =10 0.001 +5 0.005 +  
= 0.04W  
(
)
(
)
Q
10  
Total power dissipation is 0.68 + 0.15 + 0.04 = 0.87W.  
1374fb  
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and staying there. The overall loop has a gain of 74dB at  
low frequency, rolling off to unity-gain at 100kHz. Phase  
showsatwo-polecharacteristicuntiltheESRoftheoutput  
capacitor brings it back above 10kHz. Phase margin is  
about 75° at unity-gain.  
Error amplifier transconductance phase and gain are  
shown in Figure 11. The error amplifier can be modeled  
as a transconductance of 2000µMho, with an output  
impedance of 200kin parallel with 12pF. In all practical  
applications, the compensation network from VC pin to  
ground has a much lower impedance than the output  
impedance of the amplifier at frequencies above 500Hz.  
This means that the error amplifier characteristics them-  
selvesdonotcontributeexcessphaseshifttotheloop,and  
the phase/gain characteristics of the error amplifier sec-  
tion are completely controlled by the external compensa-  
tion network.  
Analog experts will note that around 4.4kHz, phase dips  
very close to the zero phase margin line. This is typical of  
switching regulators, especially those that operate over a  
wide range of loads. This region of low phase is not a  
problem as long as it does not occur near unity-gain. In  
practice, the variability of output capacitor ESR tends to  
dominate all other effects with respect to loop response.  
Variations in ESR will cause unity-gain to move around,  
but at the same time phase moves with it so that adequate  
phase margin is maintained over a very wide range of ESR  
(≥ ±3:1).  
In Figure 12, full loop phase/gain characteristics are  
shown with a compensation capacitor of 1.5nF, giving the  
erroramplifierapoleat530Hz,withphaserollingoffto90°  
LT1374  
3000  
2500  
2000  
1500  
1000  
500  
200  
150  
100  
50  
CURRENT MODE  
POWER STAGE  
m
V
SW  
FB  
OUTPUT  
PHASE  
GAIN  
ERROR  
g
= 5.3A/V  
AMPLIFIER  
R1  
R2  
ESR  
C1  
+
V
C
2.42V  
C
R
OUT  
12pF  
OUT  
200k  
+
V
2 × 10–3  
(
)
FB  
V
C
GND  
ERROR AMPLIFIER EQUIVALENT CIRCUIT  
= 50Ω  
0
R
C
R
C
F
LOAD  
1k  
–50  
C
C
100  
10k  
100k  
1M  
10M  
FREQUENCY (Hz)  
1374 F11  
1374 F09  
Figure 9. Model for Loop Response  
Figure 11. Error Amplifier Gain and Phase  
40  
20  
0
40  
80  
60  
200  
150  
100  
50  
V
V
I
= 10V  
IN  
= 5V  
= 2A  
OUT  
OUT  
GAIN  
GAIN  
0
40  
–40  
–80  
–120  
PHASE  
20  
PHASE  
V
V
C
C
= 10V  
OUT  
OUT  
–20  
–40  
IN  
0
0
= 5V, I  
= 2A  
= 100µF, 10V, AVX TPS  
= 1.5nF, R = 0, L = 10µH  
OUT  
C
C
–20  
–50  
10  
100  
1k  
10k  
100k  
1M  
10  
100  
1k  
10k  
100k  
1M  
FREQUENCY (Hz)  
FREQUENCY (Hz)  
1374 F10  
1374 F12  
Figure 10. Response from VC Pin to Output  
Figure 12. Overall Loop Characteristics  
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What About a Resistor in the Compensation Network?  
R G  
V V  
ESR 2.4  
( )( MA)(  
OUT)(  
)(  
)
C
IN  
It is common practice in switching regulator design to  
add a “zero” to the error amplifier compensation to  
increase loop phase margin. This zero is created in the  
external network in the form of a resistor (RC) in series  
with the compensation capacitor. Increasing the size of  
this resistor generally creates better and better loop  
stability, but there are two limitations on its value. First,  
the combination of output capacitor ESR and a large  
value for RC may cause loop gain to stop rolling off  
altogether, creating a gain margin problem. An approxi-  
mate formula for RC where gain margin falls to zero is:  
VC(RIPPLE  
=
)
V L f  
( )( )( )  
IN  
GMA = Error amplifier transconductance (2000µMho)  
If a computer simulation of the LT1374 showed that a  
series compensation resistor of 3k gave best overall loop  
response, with adequate gain margin, the resulting VC pin  
ripple voltage with VIN = 10V, VOUT = 5V, ESR = 0.1,  
L = 10µH, would be:  
3k 2 103 10 5 0.1 2.4  
( )  
(
)( )(  
)
VC(RIPPLE  
=
= 0.144V  
)
10 10 106 500 103  
VOUT  
( )  
R Loop Gain = 1 =  
(
)
C
G
(
G
ESR 2.42  
MP)( MA)(  
)(  
)
This ripple voltage is high enough to possibly create  
subharmonic switching. In most situations a compromise  
value (<2k in this case) for the resistor gives acceptable  
phase margin and no subharmonic problems. In other  
cases, the resistor may have to be larger to get acceptable  
phaseresponse, andsomemeansmustbeusedtocontrol  
ripple voltage at the VC pin. The suggested way to do this  
istoaddacapacitor(CF)inparallelwiththeRC/CC network  
on the VC pin. Pole frequency for this capacitor is typically  
set at one-fifth of switching frequency so that it provides  
significant attenuation of switching ripple, but does not  
addunacceptablephaseshiftatloopunity-gainfrequency.  
With RC = 3k,  
GMP = Transconductance of power stage = 5.3A/V  
GMA = Error amplifier transconductance = 2(10–3)  
ESR = Output capacitor ESR  
2.42 = Reference voltage  
With VOUT = 5V and ESR = 0.03, a value of 6.5k for RC  
wouldyieldzerogainmargin, sothisrepresentsanupper  
limit. There is a second limitation however which has  
nothing to do with theoretical small signal dynamics.  
This resistor sets high frequency gain of the error ampli-  
fier, including the gain at the switching frequency. If  
switching frequency gain is high enough, output ripple  
voltage will appear at the VC pin with enough amplitude  
to muck up proper operation of the regulator. In the  
marginal case, subharmonic switching occurs, as evi-  
denced by alternating pulse widths seen at the switch  
node. In more severe cases, the regulator squeals or  
hisses audibly even though the output voltage is still  
roughly correct. None of this will show on a theoretical  
Bode plot because Bode is an amplitude insensitive  
analysis. TestshaveshownthatifripplevoltageontheVC  
is held to less than 100mVP-P, the LT1374 will be well  
behaved. The formula below will give an estimate of VC  
ripple voltage when RC is added to the loop, assuming  
that RC is large compared to the reactance of CC at  
500kHz.  
5
5
CF =  
=
= 531pF  
( )( )( ) 2π 500 103 3k  
2π f R  
C
( )  
How Do I Test Loop Stability?  
The “standard” compensation for LT1374 is a 1.5nF  
capacitor for CC, with RC = 0. While this compensation will  
work for most applications, the “optimum” value for loop  
compensationcomponentsdepends,tovariousextent,on  
parameters which are not well controlled. These include  
inductor value (±30% due to production tolerance, load  
1374fb  
23  
LT1374  
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APPLICATIONS INFORMATION  
current and ripple current variations), output capacitance  
(±20% to ±50% due to production tolerance, tempera-  
ture, aging and changes at the load), output capacitor ESR  
(±200% due to production tolerance, temperature and  
aging), and finally, DC input voltage and output load  
current . This makes it important for the designer to check  
outthefinaldesigntoensurethatitisrobustandtolerant  
of all these variations.  
After verifying that the setup is working correctly, I start  
varying load current and input voltage to see if I can find  
any combination that makes the transient response look  
suspiciously “ringy.” This procedure may lead to an ad-  
justment for best loop stability or faster loop transient  
response. Nearly always you will find that loop response  
looks better if you add in several kfor RC. Do this only  
if necessary, because as explained before, RC above 1k  
may require the addition of CF to control VC pin ripple.  
If everything looks OK, I use a heat gun and cold spray on  
the circuit (especially the output capacitor) to bring out  
any temperature-dependent characteristics.  
I check switching regulator loop stability by pulse loading  
the regulator output while observing transient response at  
the output, using the circuit shown in Figure 13. The  
regulator loop is “hit” with a small transient AC load  
current at a relatively low frequency, 50Hz to 1kHz. This  
causes the output to jump a few millivolts, then settle back  
totheoriginalvalue,asshowninFigure14. Awellbehaved  
loop will settle back cleanly, whereas a loop with poor  
phase or gain margin will “ring” as it settles. The number  
ofringsindicatesthedegreeofstability, andthefrequency  
of the ringing shows the approximate unity-gain fre-  
quency of the loop. Amplitude of the signal is not particu-  
larlyimportant, aslongastheamplitudeisnotsohighthat  
the loop behaves nonlinearly.  
Keep in mind that this procedure does not take initial  
component tolerance into account. You should see fairly  
cleanresponseunderallloadandlineconditionstoensure  
that component variations will not cause problems. One  
note here: according to Murphy, the component most  
V
OUT AT  
I
OUT = 500mA  
BEFORE FILTER  
VOUT AT  
I
OUT = 500mA  
10mV/DIV  
5A/DIV  
AFTER FILTER  
The output of the regulator contains both the desired low  
frequency transient information and a reasonable amount  
of high frequency (500kHz) ripple. The ripple makes it  
difficult to observe the small transient, so a two-pole,  
100kHz filter has been added. This filter is not particularly  
critical; even if it attenuated the transient signal slightly,  
this wouldn’t matter because amplitude is not critical.  
VOUT AT  
IOUT = 50mA  
AFTER FILTER  
LOAD PULSE  
THROUGH 50Ω  
f 780Hz  
0.2ms/DIV  
1374 F14  
Figure 14. Loop Stability Check  
RIPPLE FILTER  
470Ω  
4.7k  
TO X1  
OSCILLOSCOPE  
PROBE  
SWITCHING  
REGULATOR  
+
100µF TO  
1000µF  
3300pF  
330pF  
50Ω  
ADJUSTABLE  
INPUT SUPPLY  
ADJUSTABLE  
DC LOAD  
TO  
OSCILLOSCOPE  
SYNC  
100Hz TO 1kHz  
100mV TO 1V  
P-P  
1374 F13  
Figure 13. Loop Stability Test Circuit  
1374fb  
24  
LT1374  
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APPLICATIONS INFORMATION  
likely to be changed in production is the output capacitor,  
because that is the component most likely to have manu-  
facturer variations (in ESR) large enough to cause prob-  
lems. It would be a wise move to lock down the sources of  
the output capacitor in production.  
Inverting regulators differ from buck regulators in the  
basicswitchingnetwork. Currentisdeliveredtotheoutput  
as square waves with a peak-to-peak amplitude much  
greater than load current. This means that maximum load  
current will be significantly less than the LT1374’s 4.5A  
maximumswitchcurrent, evenwithlargeinductorvalues.  
The buck converter in comparison, delivers current to the  
output as a triangular wave superimposed on a DC level  
equal to load current, and load current can approach 4.5A  
withlargeinductors.Outputripplevoltageforthepositive-  
to-negative converter will be much higher than a buck  
converter. Ripple current in the output capacitor will also  
be much higher. The following equations can be used to  
calculateoperatingconditionsforthepositive-to-negative  
converter.  
A possible exception to the “clean response” rule is at very  
light loads, as evidenced in Figure 14 with ILOAD = 50mA.  
Switching regulators tend to have dramatic shifts in loop  
response at very light loads, mostly because the inductor  
currentbecomesdiscontinuous.Onecommonresultisvery  
slow but stable characteristics. A second possibility is low  
phase margin, as evidenced by ringing at the output with  
transients. The good news is that the low phase margin at  
lightloadsisnotparticularlysensitivetocomponentvaria-  
tion, so if it looks reasonable under a transient test, it will  
probably not be a problem in production. Note that fre-  
quency of the light load ringing may vary with component  
tolerance but phase margin generally hangs in there.  
Maximum load current:  
V
V
(
)(  
)
IN OUT  
I −  
V
V −  
0.35  
(
)(  
)
P
OUT IN  
2 V  
+ V f L  
(
)( )( )  
OUT  
IN  
POSITIVE-TO-NEGATIVE CONVERTER  
I
=
MAX  
V
+V 0.35 V  
+ V  
F
(
)(  
)
OUT  
IN  
OUT  
The circuit in Figure 15 is a classic positive-to-negative  
topology using a grounded inductor. It differs from the  
standard approach in the way the IC chip derives its  
feedback signal, however, because the LT1374 accepts  
onlypositivefeedbacksignals,thegroundpinmustbetied  
to the regulated negative output. A resistor divider to  
ground or, in this case, the sense pin, then provides the  
proper feedback voltage for the chip.  
IP = Maximum rated switch current  
VIN = Minimum input voltage  
VOUT = Output voltage  
VF = Catch diode forward voltage  
0.35 = Switch voltage drop at 4.5A  
Example: with VIN(MIN) = 5.5V, VOUT = 5V, L = 10µH,  
VF =0.5V,IP =4.5A:IMAX =2A.Notethatthisequationdoes  
not take into account that maximum rated switch current  
(IP) on the LT1374 is reduced slightly for duty cycles  
above 50%. If duty cycle is expected to exceed 50% (input  
voltage less than output voltage), use the actual IP value  
from the Electrical Characteristics table.  
D1  
CMDSH-3  
C2  
0.27µF  
L1*  
5µH  
INPUT  
5.5V TO  
20V  
BOOST  
V
V
IN  
SW  
LT1374-5  
SENSE  
+
C3  
10µF TO  
50µF  
Operating duty cycle:  
GND  
V
C
C1  
+
100µF  
10V TANT  
×2  
C
C
C
V
OUT + VF  
D2  
MBRS330T3  
DC =  
R
V 0.3 + VOUT + VF  
OUTPUT**  
IN  
–5V, 1.8A  
* INCREASE L1 TO 10µH OR 20µH FOR HIGHER CURRENT APPLICATIONS.  
SEE APPLICATIONS INFORMATION  
** MAXIMUM LOAD CURRENT DEPENDS ON MINIMUM INPUT VOLTAGE  
AND INDUCTOR SIZE. SEE APPLICATIONS INFORMATION  
(This formula uses an average value for switch loss, so it  
may be several percent in error.)  
1374 F15  
Figure 15. Positive-to-Negative Converter  
1374fb  
25  
LT1374  
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APPLICATIONS INFORMATION  
With the conditions above:  
5 + 0.5  
lowest value of inductance that can be used, but in some  
cases (lower output load currents) it may give a value that  
creates unnecessarily high output ripple voltage. A com-  
promise value is often chosen that reduces output ripple.  
As you can see from the graph, large inductors will not  
give arbitrarily low ripple, but small inductors can give  
high ripple.  
DC =  
= 51%  
5.5 0.3 + 5 + 0.5  
This duty cycle is close enough to 50% that IP can be  
assumed to be 4.5A.  
The difficulty in calculating the minimum inductor size  
needed is that you must first know whether the switcher  
will be in continuous or discontinuous mode at the critical  
point where switch current is 4.5A. The first step is to use  
the following formula to calculate the load current where  
the switcher must use continuous mode. If your load  
current is less than this, use the discontinuous mode  
formula to calculate minimum inductor needed. If load  
current is higher, use the continuous mode formula.  
OUTPUT DIVIDER  
If the adjustable part is used, the resistor connected to  
VOUT (R2) should be set to approximately 5k. R1 is  
calculated from:  
R2 V  
– 2.42  
(
)
OUT  
R1=  
2.42  
INDUCTOR VALUE  
Output current where continuous mode is needed:  
Unlike buck converters, positive-to-negative converters  
cannot use large inductor values to reduce output ripple  
voltage. At 500kHz, values larger than 25µH make almost  
no change in output ripple. The graph in Figure 16 shows  
peak-to-peak output ripple voltage for a 5V to 5V con-  
verter versus inductor value. The criteria for choosing the  
inductor is therefore typically based on ensuring that peak  
switch current rating is not exceeded. This gives the  
2
V
2 I  
( ) ( P)  
IN  
ICONT  
=
4 V + V  
V + V + V  
IN OUT F  
(
OUT)(  
)
IN  
Minimum inductor discontinuous mode:  
2 V  
I
(
OUT)( OUT  
)
LMIN  
=
2
f I  
( )( P)  
250  
5V TO – 5V CONVERTER  
OUTPUT CAPACITOR’S  
ESR = 0.05Ω  
Minimum inductor continuous mode:  
200  
V
V
OUT  
( )(  
)
IN  
150  
LMIN  
=
I
= 1A  
LOAD  
V
+ VF  
(
)
OUT  
100  
50  
0
2 f V + V  
I I  
1+  
( )(  
)
IN  
OUT  
P
OUT  
V
IN  
I
= 0.25A  
LOAD  
For the example above, with maximum load current of 1A:  
0
5
10  
15  
20  
INDUCTOR SIZE (µH)  
2
2
)
1374 F16  
5.5 4.5  
(
) (  
I
=
= 1.15A  
CONT  
4 5.5 + 5 5.5 +5 +0.5  
Figure 16. Ripple Voltage on Positive-to-Negative Converter  
(
)(  
)
1374fb  
26  
LT1374  
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APPLICATIONS INFORMATION  
This says that discontinuous mode can be used and the  
minimum inductor needed is found from:  
somewhat higher ripple current, especially in discontinu-  
ous mode. The exact formulas are very complex and  
appear in Application Note 44, pages 30 and 31. For our  
purposes here I have simply added a fudge factor (ff). The  
value for ff is about 1.2 for higher load currents and  
L 10µH. It increases to about 2.0 for smaller inductors at  
lower load currents.  
2 5 1  
( )( )  
LMIN  
=
= 1µH  
2
500 103 4.5  
(
)
Inpractice,theinductorshouldbeincreasedbyabout30%  
over the calculated minimum to handle losses and varia-  
tionsinvalue. Thissuggestsaminimuminductorof1.3µH  
for this application, but looking at the ripple voltage chart  
showsthatoutputripplevoltagecouldbereducedbyafac-  
toroftwobyusinga15µHinductor.Thereisnoruleofthumb  
heretomakeafinaldecision.Ifmodestrippleisneededand  
the larger inductor does the trick, go for it. If ripple is non-  
critical use the smaller inductor. If ripple is extremely criti-  
cal, a second filter may have to be added in any case, and  
the lower value of inductance can be used. Keep in mind  
thattheoutputcapacitoristheothercriticalfactorindeter-  
mining output ripple voltage. Ripple shown on the graph  
(Figure16)iswithtwoparallelcapacitor’sESRof0.1.This  
isreasonableforAVXtypeTPSDorEsizesurfacemount  
solid tantalum capacitors, but the final capacitor chosen  
must be looked at carefully for ESR characteristics.  
VOUT  
Capacitor IRMS = ff I  
( )( OUT  
ff = Fudge factor (1.2 to 2.0)  
Diode Current  
)
V
IN  
Average diodecurrentisequaltoloadcurrent. Peak diode  
current will be considerably higher.  
Peak diode current:  
Continuous Mode =  
V + V  
V
V
(
)
(
)(  
)
IN  
OUT  
IN OUT  
I
+
OUT  
V
2 L f V + V  
IN  
( )( )(  
)
IN  
OUT  
2 I  
V
OUT  
(
)(  
)
OUT  
Ripple Current in the Input and Output Capacitors  
Discontinuous Mode =  
L f  
( )( )  
Positive-to-negativeconvertershavehighripplecurrentin  
both the input and output capacitors. For long capacitor  
lifetime, the RMS value of this current must be less than  
the high frequency ripple current rating of the capacitor.  
The following formula will give an approximate value for  
RMS ripple current. This formula assumes continuous  
mode and large inductor value. Small inductors will give  
Keep in mind that during start-up and output overloads,  
average diode current may be much higher than with  
normalloads.Careshouldbeusedifdiodesratedlessthan  
3A are used, especially if continuous overload conditions  
must be tolerated.  
1374fb  
27  
LT1374  
APPLICATIONS INFORMATION  
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FE Package  
16-Lead Plastic TSSOP (4.4mm)  
(Reference LTC DWG # 05-08-1663,  
Exposed Pad Variation BB)  
4.95 – 5.05*  
(.196 – .204)  
3.8  
(.149)  
16 1514 13 12 1110  
9
6.60 ±0.10  
EXPOSED  
PAD HEAT SINK  
ON BOTTOM OF  
PACKAGE  
4.50 ±0.10  
3.0  
6.25 – 6.50  
(.118) (.246 – .256)  
0.45 ±0.05  
1.05 ±0.10  
0.65 BSC  
5
7
8
1
2
3
4
6
RECOMMENDED SOLDER PAD  
1.15  
(.0453)  
MAX  
4.30 – 4.48*  
(.169 – .176)  
0° – 8°  
0.65  
(.0256)  
BSC  
0.50 – 0.70  
(.020 – .028)  
0.105 – 0.180  
(.0041 – .0071)  
0.05 – 0.15  
(.002 – .006)  
FE16 TSSOP 1101  
0.195 – 0.30  
(.0077 – .0118)  
NOTE:  
1. CONTROLLING DIMENSION: MILLIMETERS  
MILLIMETERS  
2. DIMENSIONS ARE IN  
(INCHES)  
3. DRAWING NOT TO SCALE  
*DIMENSIONS DO NOT INCLUDE MOLD FLASH. MOLD FLASH  
SHALL NOT EXCEED 0.150mm (.006") PER SIDE  
1374fb  
28  
LT1374  
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PACKAGE DESCRIPTION  
R Package  
7-Lead Plastic DD Pak  
(LTC DWG # 05-08-1462)  
0.060  
(1.524)  
TYP  
0.390 – 0.415  
(9.906 – 10.541)  
0.060  
(1.524)  
0.165 – 0.180  
(4.191 – 4.572)  
0.256  
(6.502)  
0.045 – 0.055  
(1.143 – 1.397)  
15° TYP  
+0.008  
0.004  
–0.004  
0.060  
(1.524)  
0.059  
(1.499)  
TYP  
0.183  
(4.648)  
0.330 – 0.370  
(8.382 – 9.398)  
+0.203  
–0.102  
0.102  
(
)
0.095 – 0.115  
(2.413 – 2.921)  
0.075  
(1.905)  
0.040 – 0.060  
(1.016 – 1.524)  
0.026 – 0.036  
(0.660 – 0.914)  
0.050 ± 0.012  
(1.270 ± 0.305)  
0.300  
(7.620)  
0.013 – 0.023  
(0.330 – 0.584)  
+0.012  
0.143  
–0.020  
+0.305  
BOTTOM VIEW OF DD PAK  
HATCHED AREA IS SOLDER PLATED  
COPPER HEAT SINK  
3.632  
(
)
–0.508  
R (DD7) 0396  
1374fb  
29  
LT1374  
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PACKAGE DESCRIPTION  
S8 Package  
8-Lead Plastic Small Outline (Narrow 0.150)  
(LTC DWG # 05-08-1610)  
0.189 – 0.197*  
(4.801 – 5.004)  
7
5
8
6
0.150 – 0.157**  
(3.810 – 3.988)  
0.228 – 0.244  
(5.791 – 6.197)  
1
0.053 – 0.069  
3
4
2
0.010 – 0.020  
(0.254 – 0.508)  
× 45°  
(1.346 – 1.752)  
0.004 – 0.010  
(0.101 – 0.254)  
0.008 – 0.010  
(0.203 – 0.254)  
0°– 8° TYP  
0.016 – 0.050  
0.406 – 1.270  
0.050  
(1.270)  
TYP  
0.014 – 0.019  
(0.355 – 0.483)  
*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  
SO8 0996  
1374fb  
30  
LT1374  
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PACKAGE DESCRIPTION  
T7 Package  
7-Lead Plastic TO-220 (Standard)  
(LTC DWG # 05-08-1422)  
0.165 – 0.180  
(4.191 – 4.572)  
0.147 – 0.155  
(3.734 – 3.937)  
DIA  
0.390 – 0.415  
(9.906 – 10.541)  
0.045 – 0.055  
(1.143 – 1.397)  
0.230 – 0.270  
(5.842 – 6.858)  
0.570 – 0.620  
(14.478 – 15.748)  
0.620  
(15.75)  
TYP  
0.460 – 0.500  
(11.684 – 12.700)  
0.330 – 0.370  
(8.382 – 9.398)  
0.700 – 0.728  
(17.780 – 18.491)  
0.095 – 0.115  
(2.413 – 2.921)  
0.152 – 0.202  
(3.860 – 5.130)  
0.260 – 0.320  
(6.604 – 8.128)  
0.013 – 0.023  
(0.330 – 0.584)  
0.040 – 0.060  
(1.016 – 1.524)  
0.026 – 0.036  
(0.660 – 0.914)  
0.135 – 0.165  
(3.429 – 4.191)  
0.155 – 0.195  
(3.937 – 4.953)  
T7 (TO-220) (FORMED) 1197  
1374fb  
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 represen-  
tationthattheinterconnectionofitscircuitsasdescribedhereinwillnotinfringeonexistingpatentrights.  
31  
LT1374  
U
TYPICAL APPLICATION  
Dual Output SEPIC Converter  
losses. C4 provides a low impedance path to maintain an  
equal voltage swing in L1B, improving regulation. In a  
flybackconverter,duringswitchontime,alltheconverter’s  
energyisstoredinL1Aonly, sincenocurrentflowsinL1B.  
At switch off, energy is transferred by magnetic coupling  
into L1B, powering the 5V rail. C4 pulls L1B positive  
duringswitchontime, causingcurrenttoflow, andenergy  
to build in L1B and C4. At switch off, the energy stored in  
both L1B and C4 supply the 5V rail. This reduces the  
current in L1A and changes L1B current waveform from  
square to triangular. For details on this circuit see Design  
Note 100.  
The circuit in Figure 17 generates both positive and  
negative 5V outputs with a single piece of magnetics. The  
two inductors shown are actually just two windings on a  
standard BH Electronics inductor. The topology for the 5V  
output is a standard buck converter. The 5V topology  
would be a simple flyback winding coupled to the buck  
converter if C4 were not present. C4 creates the SEPIC  
(Single-Ended Primary Inductance Converter) topology  
which improves regulation and reduces ripple current in  
L1. Without C4, the voltage swing on L1B compared to  
L1A would vary due to relative loading and coupling  
C2  
0.27µF  
D2  
CMDSH-3  
BOOST  
INPUT  
OUTPUT  
5V  
V
V
SW  
IN  
6V TO 25V  
L1A*  
LT1374-5 BIAS  
SENSE  
6.8µH  
SHDN  
GND  
V
C
+
+
C1**  
100µF  
R
C
10V TANT  
+
C3  
22µF  
470Ω  
D1  
MBRD340  
C
C
35V TANT  
0.01µF  
GND  
+
C5**  
100µF  
10V TANT  
C4**  
4.7nF  
* L1 IS A SINGLE CORE WITH TWO WINDINGS  
BH ELECTRONICS #501-0726  
L1B*  
D3  
MBRD340  
** TOKIN IE475ZY5U-C304  
OUTPUT  
IF LOAD CAN GO TO ZERO, AN OPTIONAL  
–5V  
PRELOAD OF 1k TO 5k MAY BE USED TO  
IMPROVE LOAD REGULATION  
1374 F17  
Figure 17. Dual Output SEPIC Converter  
RELATED PARTS  
PART NUMBER  
LT1074/LT1076  
LTC®1148  
LTC1149  
DESCRIPTION  
COMMENTS  
Step-Down Switching Regulators  
40V Input, 100kHz, 5A and 2A  
External FET Switches  
High Efficiency Synchronous Step-Down Switching Regulator  
High Efficiency Synchronous Step-Down Switching Regulator  
High Efficiency Step-Down and Inverting DC/DC Converter  
Step-Down Switching Regulator  
External FET Switches  
LTC1174  
0.5A, 150kHz Burst Mode® Operation  
PDIP LT1076  
LT1176  
LT1370  
High Efficiency DC/DC Converter  
42V, 6A, 500kHz Switch  
LT1371  
High Efficiency DC/DC Converter  
35V, 3A, 500kHz Switch  
LT1372/LT1377  
LTC1735  
500kHz and 1MHz High Efficiency 1.5A Switching Regulators  
High Efficiency Step-Down Converter  
Boost Topology  
External Switches, Very High Efficiency  
1.25MHz, 3A, 25V Input, SO-8 and TSSOP16 Packages  
200kHz, 1.5A, 60V Input, SO-8 and GN16 Packages  
1.25MHz, 1.5A, 25V Input, MS8 Package  
LT1765  
3A Step-Down Switching Regulator  
LT1766  
1.5A Step-Down Switching Regulator  
LT1767  
1.5A Step-Down Switching Regulator  
Burst Mode is a registered trademark of Linear Technology Corporation.  
1374fb  
LT/TP 0102 1.5K REV B • PRINTED IN USA  
LinearTechnology Corporation  
1630 McCarthy Blvd., Milpitas, CA 95035-7417  
32  
(408) 432-1900 FAX: (408) 434-0507 www.linear.com  
LINEAR TECHNOLOGY CORPORATION 1998  

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Linear

LT1374CR-5#PBF

LT1374 - 4.5A, 500kHz Step-Down Switching Regulator; Package: DD PAK; Pins: 7; Temperature Range: 0&deg;C to 70&deg;C
Linear

LT1374CR-5#TR

LT1374 - 4.5A, 500kHz Step-Down Switching Regulator; Package: DD PAK; Pins: 7; Temperature Range: 0&deg;C to 70&deg;C
Linear

LT1374CR-5#TRPBF

LT1374 - 4.5A, 500kHz Step-Down Switching Regulator; Package: DD PAK; Pins: 7; Temperature Range: 0&deg;C to 70&deg;C
Linear

LT1374CR-5SYNC

4.5A, 500kHz Step-Down Switching Regulator
Linear

LT1374CR-5SYNC#TR

IC 8.5 A SWITCHING REGULATOR, 560 kHz SWITCHING FREQ-MAX, PSSO7, PLASTIC, D2PAK-7, Switching Regulator or Controller
Linear

LT1374CR-5SYNC#TRPBF

IC 8.5 A SWITCHING REGULATOR, 560 kHz SWITCHING FREQ-MAX, PSSO7, PLASTIC, D2PAK-7, Switching Regulator or Controller
Linear

LT1374CR-SYNC

4.5A, 500kHz Step-Down Switching Regulator
Linear

LT1374CR-SYNC#PBF

LT1374 - 4.5A, 500kHz Step-Down Switching Regulator; Package: DD PAK; Pins: 7; Temperature Range: 0&deg;C to 70&deg;C
Linear

LT1374CR-SYNC#TR

IC 8.5 A SWITCHING REGULATOR, 560 kHz SWITCHING FREQ-MAX, PSSO7, PLASTIC, D2PAK-7, Switching Regulator or Controller
Linear

LT1374CS8

4.5A, 500kHz Step-Down Switching Regulator
Linear

LT1374CS8#PBF

LT1374 - 4.5A, 500kHz Step-Down Switching Regulator; Package: SO; Pins: 8; Temperature Range: 0&deg;C to 70&deg;C
Linear