ADP1173AR

更新时间:2024-09-18 02:10:44
品牌:ADI
描述:Micropower DC-DC Converter

ADP1173AR 概述

Micropower DC-DC Converter 微功率DC- DC转换器

ADP1173AR 数据手册

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Micropower  
DC-DC Converter  
a
ADP1173  
FUNCTIONAL BLOCK DIAGRAMS  
FEATURES  
Operates From 2.0 V to 30 V Input Voltages  
Only 110 A Supply Current (Typical)  
Step-Up or Step-Down Mode Operation  
Very Few External Components Required  
Low Battery Detector On-Chip  
User-Adjustable Current Limit  
Internal 1 A Power Switch  
SET  
ADP1173  
A2  
AO  
V
IN  
GAIN BLOCK/  
ERROR AMP  
I
LIM  
SW1  
1.245V  
REFERENCE  
Fixed or Adjustable Output Voltage Versions  
8-Pin DIP or SO-8 Package  
A1  
COMPARATOR  
OSCILLATOR  
DRIVER  
APPLICATIONS  
Notebook and Palmtop Computers  
Cellular Telephones  
SW2  
GND  
FB  
Flash Memory Vpp Generators  
3 V to 5 V, 5 V to 12 V Converters  
9 V to 5 V, 12 V to 5 V Converters  
Portable Instruments  
SET  
ADP1173-3.3  
ADP1173-5  
ADP1173-12  
LCD Bias Generators  
A2  
AO  
V
IN  
GENERAL DESCRIPTION  
GAIN BLOCK/  
ERROR AMP  
I
LIM  
The ADP1173 is part of a family of step-up/step-down switching  
regulators that operates from an input supply voltage of as little as  
2 V to 12 V in step-up mode and to 30 V in step-down mode.  
SW1  
1.245V  
REFERENCE  
A1  
COMPARATOR  
OSCILLATOR  
DRIVER  
SW2  
The ADP1173 consumes as little as 110 µA in standby mode,  
making it ideal for applications that need low quiescent current.  
An auxiliary gain amplifier can serve as a low battery detector,  
linear regulator (under voltage lockout) or error amplifier.  
R1  
ADP1173-3.3: R1 = 456k  
ADP1173-5: R1 = 250kΩ  
ADP1173-12: R1 = 87.4kΩ  
R2  
753kΩ  
GND  
SENSE  
The ADP1173 can deliver 80 mA at 5 V from a 3 V input in  
step-up configuration or 100 mA at 5 V from a 12 V input in  
step-down configuration. For input voltages of less than 2 V use  
the ADP1073.  
REV. 0  
Information furnished by Analog Devices is believed to be accurate and  
reliable. However, no responsibility is assumed by Analog Devices for its  
use, nor for any infringements of patents or other rights of third parties  
which may result from its use. No license is granted by implication or  
otherwise under any patent or patent rights of Analog Devices.  
One Technology Way, P.O. Box 9106, Norwood, MA 02062-9106, U.S.A.  
Tel: 617/329-4700  
Fax: 617/326-8703  
World Wide Web Site: http://www.analog.com  
© Analog Devices, Inc., 1997  
ADP1173–SPECIFICATIONS (@ T = 0؇C to +70؇C, V = 3 V unless otherwise noted)  
A
IN  
Model  
Symbol Conditions  
Min  
Typ  
Max  
Units  
QUIESCENT CURRENT  
IQ  
Switch Off  
110  
150  
µA  
QUIESCENT CURRENT, BOOST MODE IQ  
CONFIGURATION  
No Load, TA = +25°C  
ADP1173-3.3  
ADP1173-5  
135  
135  
250  
µA  
µA  
µA  
ADP1173-12  
INPUT VOLTAGE  
VIN  
Step-Up Mode  
Step-Down Mode  
2.0  
12.6  
30  
V
V
COMPARATOR TRIP POINT VOLTAGE  
OUTPUT SENSE VOLTAGE  
ADP11731  
1.20  
1.245  
1.30  
V
VOUT  
ADP1173-3.32  
ADP1173-52  
ADP1173-122  
3.14  
4.75  
11.4  
3.30  
5.00  
12.0  
3.46  
5.25  
12.6  
V
V
V
COMPARATOR HYSTERESIS  
OUTPUT HYSTERESIS  
ADP1173  
5
12  
mV  
ADP1173-3.3  
ADP1173-5  
ADP1173-12  
13  
20  
50  
35  
55  
100  
mV  
mV  
mV  
OSCILLATOR FREQUENCY  
DUTY CYCLE  
fOSC  
16  
43  
15  
24  
32  
kHz  
%
Full Load  
55  
63  
SWITCH ON TIME  
tON  
ILIM Tied to VIN  
23  
32  
µs  
FEEDBACK PIN BIAS CURRENT  
SET PIN BIAS CURRENT  
GAIN BLOCK OUTPUT LOW  
REFERENCE LINE REGULATION  
ADP1173, VFB = 0 V  
VSET = VREF  
60  
290  
150  
0.4  
nA  
nA  
V
70  
VOL  
ISINK = 100 µA, VSET = 1.00 V  
0.15  
2.0 V VIN 5 V  
5 V VIN 30 V  
0.2  
0.02  
0.4  
0.075  
%/V  
%/V  
SWSAT VOLTAGE, STEP-UP MODE  
VSAT  
VIN = 3.0 V, ISW = 650 mA  
0.5  
0.8  
0.85  
V
V
IN = 5.0 V, ISW = 1 A,  
TA = +25°C  
VIN = 5.0 V, ISW = 1 A  
1.0  
1.4  
V
V
SWSAT VOLTAGE, STEP-DOWN MODE  
VSAT  
VIN = 12 V, TA = +25°C,  
I
SW = 650 mA  
1.1  
1.5  
1.7  
V
V
VIN = 12 V, ISW = 650 mA  
GAIN BLOCK GAIN  
CURRENT LIMIT  
AV  
RL = 100 k3  
400  
1000  
400  
V/V  
mA  
220 from ILIM to VIN  
TA = +25°C  
CURRENT LIMIT TEMPERATURE  
COEFFICIENT  
–0.3  
1
%/°C  
µA  
SWITCH-OFF LEAKAGE CURRENT  
Measured at SW1 Pin  
10  
TA = +25°C  
MAXIMUM EXCURSION BELOW GND VSW2  
I
SW1 10 µA, Switch Off  
–400  
–350  
mV  
TA = +25°C  
NOTES  
1This specification guarantees that both the high and low trip points of the comparator fall within the 1.20 V to 1.30 V range.  
2The output voltage waveform will exhibit a sawtooth shape due to the comparator hysteresis. The output voltage on the fixed output versions will always be within  
the specified range.  
3100 kresistor connected between a 5 V source and the AO pin.  
Specifications subject to change without notice.  
REV. 0  
–2–  
ADP1173  
ABSOLUTE MAXIMUM RATINGS*  
PIN CONFIGURATIONS  
Supply Voltage (VIN) . . . . . . . . . . . . . . . . . . . . . . . . . . . . 36 V  
SW1 Pin Voltage (VSW1) . . . . . . . . . . . . . . . . . . . . . . . . . 50 V  
SW2 Pin Voltage (VSW2) . . . . . . . . . . . . . . . . . . –0.5 V to VIN  
Feedback Pin Voltage (ADP1173) . . . . . . . . . . . . . . . . . . . 5 V  
Sense Pin Voltage (ADP1173, –3.3, –5, –12) . . . . . . . . . 36 V  
Maximum Power Dissipation . . . . . . . . . . . . . . . . . . 500 mW  
Maximum Switch Current . . . . . . . . . . . . . . . . . . . . . . . .1.5 A  
Operating Temperature Range . . . . . . . . . . . . . 0°C to +70°C  
Storage Temperature Range . . . . . . . . . . . . . –65°C to 150°C  
Lead Temperature, (Soldering, 10 sec) . . . . . . . . . . . .+300°C  
N-8  
SO-8  
8-Lead Plastic SO  
8-Lead Plastic DIP  
I
1
2
3
4
8
7
6
5
FB (SENSE)*  
SET  
I
1
2
3
4
8
7
6
5
FB (SENSE)*  
SET  
LIM  
LIM  
ADP1173  
ADP1173  
V
V
IN  
IN  
TOP VIEW  
(Not to Scale)  
TOP VIEW  
(Not to Scale)  
SW1  
SW2  
AO  
SW1  
SW2  
AO  
GND  
GND  
*FIXED VERSIONS  
*FIXED VERSIONS  
*Stresses above those listed under Absolute Maximum Ratings may cause perma-  
nent damage to the device. This is a stress rating only; functional operation of the  
device at these or any other conditions above those listed in the operational  
sections of this specification is not implied. Exposure to absolute maximum  
ratings for extended periods of time may affect device reliability.  
PIN FUNCTION DESCRIPTIONS  
Function  
Mnemonic  
ILIM  
For normal conditions this pin is connected to  
VIN. When lower current is required, a resistor  
should be connected between ILIM and VIN.  
Limiting the switch current to 400 mA is  
achieved by connecting a 220 resistor.  
ORDERING GUIDE  
Output  
Voltage  
Package  
Options*  
Model  
ADP1173AN  
ADP1173AR  
ADJ  
ADJ  
3.3 V  
3.3 V  
5 V  
5 V  
12 V  
12 V  
N-8  
SO-8  
N-8  
SO-8  
N-8  
SO-8  
N-8  
VIN  
Input Voltage.  
SW1  
Collector Node of Power Transistor.  
For step-down configuration, connect to VIN;  
for step-up configuration, connect to an  
inductor/diode.  
ADP1173AN-3.3  
ADP1173AR-3.3  
ADP1173AN-5  
ADP1173AR-5  
ADP1173AN-12  
ADP1173AR-12  
SW2  
Emitter Node of Power Transistor. For step-  
down configuration, connect to inductor/  
diode; for step-up configuration, connect to  
ground. Do not allow this pin to drop more  
than a diode drop below ground.  
SO-8  
*N = Plastic DIP, SO = Small Outline Package.  
L1*  
100µH  
IRF7203  
GND  
AO  
Ground.  
+5V  
OUTPUT  
AT 100mA  
+
Auxiliary Gain (GB) Output. The open  
56  
470µF  
collector can sink 100 µA.  
470kΩ  
2
1
75kΩ  
I
V
IN  
LIM  
SET  
Gain Amplifier Input. The amplifier has  
positive input connected to the SET pin and  
negative input is connected to 1.245 V  
reference.  
3
6
SW1  
4X NICAD  
OR  
ALKALINE  
CELLS  
ADP1173  
+
AO  
FB  
470µF  
7
SET  
8
GND SW2  
+
4
240Ω  
24kΩ  
5
470µF  
FB/SENSE  
On the ADP1173 (adjustable) version this pin  
is connected to the comparator input. On the  
ADP1173-3.3, ADP1173-5 and ADP1173-12,  
the pin goes directly to the internal application  
resistor that sets the output voltage.  
*L1 = COILTRONICS CTX100-4  
Figure 1. Step-Up or Step-Down Converter  
CAUTION  
ESD (electrostatic discharge) sensitive device. Electrostatic charges as high as 4000 V readily  
accumulate on the human body and test equipment and can discharge without detection.  
Although the ADP1173 features proprietary ESD protection circuitry, permanent damage may  
occur on devices subjected to high energy electrostatic discharges. Therefore, proper ESD  
precautions are recommended to avoid performance degradation or loss of functionality.  
WARNING!  
ESD SENSITIVE DEVICE  
REV. 0  
–3–  
ADP1173–Typical Performance Characteristics  
1.2  
1.0  
0.8  
0.6  
0.4  
0.2  
0
1.6  
1.4  
1.2  
1.0  
0.8  
0.6  
0.4  
0.2  
0.0  
1100  
1000  
900  
800  
700  
600  
500  
400  
300  
200  
100  
V
= 3V  
IN  
V
CE(SAT)  
2V < V < 5V  
IN  
V
= 2V  
IN  
V
= 5V  
IN  
10  
100  
 
1000  
0.2  
0.4  
0.6  
0.8  
1.0  
1.2  
0.05 0.15 0.25 0.35 0.45 0.55 0.65 0.75  
SWITCH CURRENT – A  
SWITCH CURRENT – A  
R
LIM  
Figure 2. Saturation Voltage vs.  
Switch Current in Step-Up Mode  
Figure 3. Switch ON Voltage vs.  
Switch Current in Step-Down Mode  
Figure 4. Maximum Switch Current  
vs. RLIM in Step-Up Mode  
1000  
120  
100  
90  
80  
70  
60  
50  
V
=24V WITH L = 500µH @ V  
= 5V  
OUT  
IN  
900  
800  
700  
600  
500  
400  
300  
200  
100  
0
110  
QUIESCENT CURRENT  
100  
90  
80  
70  
60  
50  
40  
V
= 5V  
IN  
40  
30  
20  
10  
0
V
=12V WITH L = 250µH @ V  
= 5V  
OUT  
IN  
V
= 2V  
IN  
100  
1000  
–40  
0
25  
70  
85  
0
100 200 300 400 500 600 700 800 900  
SWITCH CURRENT – mA  
R
Ω  
LIM  
TEMPERATURE – °C  
Figure 5. Maximum Switch Current  
vs. RLIM in Step-Down Mode  
Figure 6. Supply Current vs.  
Switch Current  
Figure 7. Quiescent Current vs.  
Temperature  
25.5  
25  
80  
70  
60  
450  
400  
350  
300  
250  
200  
24.5  
24  
V
= 3V  
IN  
50  
40  
23.5  
V
= 3V  
IN  
23  
150  
100  
50  
OSCILLATOR FREQUENCY  
22.5  
30  
20  
10  
22  
21.5  
0
–40  
3
5
10  
15  
20  
25  
30  
–40  
0
25  
TEMPERATURE –  
70  
85  
0
25  
70  
85  
INPUT VOLTAGE – Volts  
°
C
TEMPERATURE – °C  
Figure 9. Set Pin Bias Current vs.  
Temperature  
Figure 10. Feedback Pin Bias Current  
vs. Temperature  
Figure 8. Oscillator Frequency vs.  
Input Voltage  
REV. 0  
–4–  
ADP1173  
COMPONENT SELECTION  
APPLICATIONS  
Theory of Operation  
General Notes on Inductor Selection  
When the ADP1173 internal power switch turns on, current  
begins to flow in the inductor. Energy is stored in the inductor  
core while the switch is on, and this stored energy is then  
transferred to the load when the switch turns off. Both the  
collector and the emitter of the switch transistor are accessible  
on the ADP1173, so the output voltage can be higher, lower or  
of opposite polarity than the input voltage.  
The ADP1173 is a flexible, low power switch mode power  
supply (SMPS) controller. The regulated output voltage can be  
greater than the input voltage (boost or step-up mode) or less  
than the input (buck or step-down mode). This device uses a  
gated-oscillator technique to provide very high performance  
with low quiescent current.  
A functional block diagram of the ADP1173 is shown on the  
front page. The internal 1.245 V reference is connected to one  
input of the comparator, while the other input is externally  
connected (via the FB pin) to a feedback network connected to  
the regulated output. When the voltage at the FB pin falls below  
1.245 V, the 24 kHz oscillator turns on. A driver amplifier pro-  
vides base drive to the internal power switch, and the switching  
action raises the output voltage. When the voltage at the FB pin  
exceeds 1.245 V, the oscillator is shut off. While the oscillator is  
off, the ADP1173 quiescent current is only 110 µA. The com-  
parator includes a small amount of hysteresis, which ensures  
loop stability without requiring external components for fre-  
quency compensation.  
To specify an inductor for the ADP1173, the proper values of  
inductance, saturation current and dc resistance must be  
determined. This process is not difficult, and specific equations  
for each circuit configuration are provided in this data sheet. In  
general terms, however, the inductance value must be low  
enough to store the required amount of energy (when both  
input voltage and switch ON time are at a minimum) but high  
enough that the inductor will not saturate when both VIN and  
switch ON time are at their maximum values. The inductor  
must also store enough energy to supply the load without  
saturating. Finally, the dc resistance of the inductor should be  
low, so that excessive power will not be wasted by heating the  
windings. For most ADP1173 applications, an inductor of  
47 µH to 470 µH, with a saturation current rating of 300 mA to  
1 A and dc resistance <1 is suitable. Ferrite core inductors  
which meet these specifications are available in small, surface-  
mount packages.  
The maximum current in the internal power switch can be set  
by connecting a resistor between VIN and the ILIM pin. When the  
maximum current is exceeded, the switch is turned OFF. The  
current limit circuitry has a time delay of about 2 µs. If an  
external resistor is not used, connect ILIM to VIN. Further  
information on ILIM is included in the Limiting the Switch  
Current section of this data sheet.  
To minimize Electro-Magnetic Interference (EMI), a toroid or  
pot core type inductor is recommended. Rod core inductors are  
a lower cost alternative if EMI is not a problem.  
The ADP1173 internal oscillator provides 23 µs ON and 19 µs  
OFF times, which is ideal for applications where the ratio  
between VIN and VOUT is roughly a factor of two (such as  
converting +3 V to + 5 V). However, wider range conversions  
(such as generating +12 V from a +5 V supply) can easily be  
accomplished.  
CALCULATING THE INDUCTOR VALUE  
Selecting the proper inductor value is a simple three-step  
process:  
1. Define the operating parameters: minimum input voltage,  
maximum input voltage, output voltage and output current.  
An uncommitted gain block on the ADP1173 can be connected  
as a low battery detector. The inverting input of the gain block  
is internally connected to the 1.245 V reference. The noninvert-  
ing input is available at the SET pin. A resistor divider, con-  
nected between VIN and GND with the junction connected to  
the SET pin, causes the AO output to go LOW when the low  
battery set point is exceeded. The AO output is an open  
collector NPN transistor which can sink 100 µA.  
2. Select the appropriate conversion topology (step-up, step-  
down, or inverting).  
3. Calculate the inductor value, using the equations in the  
following sections.  
Inductor Selection—Step-Up Converter  
In a step-up, or boost, converter (Figure 14), the inductor must  
store enough power to make up the difference between the  
input voltage and the output voltage. The power that must be  
stored is calculated from the equation:  
The ADP1173 provides external connections for both the  
collector and emitter of its internal power switch, which permits  
both step-up and step-down modes of operation. For the step-  
up mode, the emitter (pin SW2) is connected to GND and the  
collector (pin SW1) drives the inductor. For step-down mode,  
the emitter drives the inductor while the collector is connected  
to VIN.  
PL = V  
+VD VIN(MIN) × I  
(1)  
(
)
(
)
OUT  
OUT  
where VD is the diode forward voltage (0.5 V for a 1N5818  
Schottky). Energy is only stored in the inductor while the  
ADP1173 switch is ON, so the energy stored in the inductor on  
each switching cycle must be must be equal to or greater than:  
PL  
The output voltage of the ADP1173 is set with two external  
resistors. Three fixed-voltage models are also available:  
ADP1173-3.3 (+3.3 V), ADP1173-5 (+5 V) and ADP1173-12  
(+12 V). The fixed-voltage models are identical to the ADP1173,  
except that laser-trimmed voltage-setting resistors are included  
on the chip. On the fixed-voltage models of the ADP1173,  
simply connect the feedback pin (Pin 8) directly to the output  
voltage.  
(2)  
fOSC  
in order for the ADP1173 to regulate the output voltage.  
REV. 0  
–5–  
ADP1173  
When the internal power switch turns ON, current flow in the  
inductor increases at the rate of:  
When selecting an inductor, the peak current must not exceed  
the maximum switch current of 1.5 A. If the equations shown  
above result in peak currents > 1.5 A, the ADP1073 should be  
considered. This device has a 72% duty cycle, so more energy is  
stored in the inductor on each cycle. This results in greater  
output power.  
Rt  
L
VIN  
R′  
IL (t)=  
1– e  
(3)  
where L is in henrys and R' is the sum of the switch equivalent  
resistance (typically 0.8 at +25°C) and the dc resistance of  
the inductor. In most applications, where the voltage drop across  
the switch is small compared to VIN , a simpler equation can be  
used:  
The peak current must be evaluated for both minimum and  
maximum values of input voltage. If the switch current is high  
when VIN is at its minimum, then the 1.5 A limit may be ex-  
ceeded at the maximum value of VIN. In this case, the ADP1173’s  
current limit feature can be used to limit switch current. Simply  
select a resistor (using Figure 4) that will limit the maximum  
switch current to the IPEAK value calculated for the minimum  
value of VIN. This will improve efficiency by producing a con-  
stant IPEAK as VIN increases. See the Limiting the Switch Current  
section of this data sheet for more information.  
VIN  
L
IL (t)=  
t
(4)  
Replacing “t” in the above equation with the ON time of the  
ADP1173 (23 µs, typical) will define the peak current for a  
given inductor value and input voltage. At this point, the  
inductor energy can be calculated as follows:  
Note that the switch current limit feature does not protect the  
circuit if the output is shorted to ground. In this case, current is  
only limited by the dc resistance of the inductor and the forward  
voltage of the diode.  
1
2
EL  
=
LI2  
(5)  
PEAK  
As previously mentioned, EL must be greater than PL/fOSC so the  
ADP1173 can deliver the necessary power to the load. For best  
efficiency, peak current should be limited to 1 A or less. Higher  
switch currents will reduce efficiency, because of increased  
saturation voltage in the switch. High peak current also increases  
output ripple. As a general rule, keep peak current as low as pos-  
sible to minimize losses in the switch, inductor and diode.  
Inductor Selection—Step-Down Converter  
The step-down mode of operation is shown in Figure 15. Unlike  
the step-up mode, the ADP1173’s power switch does not  
saturate when operating in the step-down mode. Therefore,  
switch current should be limited to 650 mA in this mode. If the  
input voltage will vary over a wide range, the ILIM pin can be  
used to limit the maximum switch current. If higher output  
current is required, the ADP1111 should be considered.  
In practice, the inductor value is easily selected using the equa-  
tions above. For example, consider a supply that will generate  
9 V at 50 mA from a 3 V source. The inductor power required  
is, from Equation 1:  
The first step in selecting the step-down inductor is to calculate  
the peak switch current as follows:  
PL =(9V +0.5V 3V )×(50 mA)= 325 mW  
On each switching cycle, the inductor must supply:  
PL 325 mW  
2IOUT  
DC VIN VSW +VD  
VOUT +VD  
IPEAK  
=
(6)  
=
=13.5µJ  
where DC = duty cycle (0.55 for the ADP1173)  
SW = voltage drop across the switch  
VD = diode drop (0.5 V for a 1N5818)  
OUT = output current  
fOSC 24 kHz  
V
The required inductor power is fairly low in this example, so the  
peak current can also be low. Assuming a peak current of 500 mA  
as a starting point, Equation 4 can be rearranged to recommend  
an inductor value:  
I
VOUT = the output voltage  
VIN = the minimum input voltage  
VIN  
3V  
L =  
t =  
23 µs =138 µH  
As previously mentioned, the switch voltage is higher in step-  
down mode than step-up mode. VSW is a function of switch  
IL(MAX ) 500 mA  
Substituting a standard inductor value of 100 µH, with 0.2 dc  
resistance, will produce a peak switch current of:  
current and is therefore a function of VIN, L, time and VOUT  
.
For most applications, a VSW value of 1.5 V is recommended.  
The inductor value can now be calculated:  
VIN(MIN) VSW VOUT  
IPEAK  
where tON = switch ON time (23 µs)  
1.0Ω × 23µs  
3V  
100 µH  
IPEAK  
=
1– e  
=616 mA  
1. 0 Ω  
L =  
× tON  
(7)  
Once the peak current is known, the inductor energy can be  
calculated from Equation 5:  
If the input voltage will vary (such as an application that must  
operate from a 12 V to 24 V source) an RLIM resistor should be  
selected from Figure 5. The RLIM resistor will keep switch cur-  
rent constant as the input voltage rises. Note that there are separate  
1
2
EL  
=
(100 µH)×(616 mA)2 =19 µJ  
The inductor energy of 19 µJ is greater than the PL/fOSC re-  
quirement of 13.5 µJ, so the 100 µH inductor will work in this  
application. By substituting other inductor values into the same  
equations, the optimum inductor value can be selected.  
RLIM values for step-up and step-down modes of operation.  
REV. 0  
–6–  
ADP1173  
For example, assume that +5 V at 300 mA is required from a  
12 V to +24 V input. Deriving the peak current from Equation 6  
yields:  
Using a standard inductor value of 220 µH, with 0.2 dc  
resistance, will produce a peak switch current of:  
–0.85Ω × 23 µs  
4.5V 0.75V  
0.65 +0.2 Ω  
220 µH  
IPEAK  
=
1– e  
= 375 mA  
2×300 mA  
5 + 0.5  
IPEAK  
=
= 545 mA  
0.55  
12 1.5+ 0.5  
Once the peak current is known, the inductor energy can be  
calculated from Equation 5:  
The peak current can then be inserted into Equation 7 to calcu-  
late the inductor value:  
1
2
(220 µH)×(375 mA)2 =15.5µJ  
12 –1.5–5  
545 mA  
EL  
=
L =  
×23 µs = 232 µH  
The inductor energy of 15.5 µJ is greater than the PL/fOSC  
requirement of 11.5 µJ, so the 220 µH inductor will work in  
this application.  
Since 232 µH is not a standard value, the next lower standard  
value of 220 µH would be specified.  
To avoid exceeding the maximum switch current when the  
input voltage is at +24 V, an RLIM resistor should be specified.  
Using the step-down curve of Figure 5, a value of 180 will  
limit the switch current to 600 mA.  
The input voltage only varies between 4.5 V and 5.5 V in this  
example. Therefore, the peak current will not change enough to  
require an RLIM resistor and the ILIM pin can be connected  
directly to VIN. Care should be taken to ensure that the peak  
current does not exceed 650 mA.  
Inductor Selection—Positive-to-Negative Converter  
The configuration for a positive-to-negative converter using the  
ADP1173 is shown in Figure 17. As with the step-up converter,  
all of the output power for the inverting circuit must be supplied  
by the inductor. The required inductor power is derived from  
the formula:  
CAPACITOR SELECTION  
For optimum performance, the ADP1173’s output capacitor  
must be carefully selected. Choosing an inappropriate capacitor  
can result in low efficiency and/or high output ripple.  
Ordinary aluminum electrolytic capacitors are inexpensive, but  
often have poor Equivalent Series Resistance (ESR) and  
Equivalent Series Inductance (ESL). Low ESR aluminum ca-  
pacitors, specifically designed for switch mode converter appli-  
cations, are also available, and these are a better choice than  
general purpose devices. Even better performance can be  
achieved with tantalum capacitors, although their cost is higher.  
Very low values of ESR can be achieved by using OS-CON*  
capacitors (Sanyo Corporation, San Diego, CA). These devices  
are fairly small, available with tape-and-reel packaging, and have  
very low ESR.  
PL = |VOUT|+VD × I  
) (  
(8)  
(
)
OUT  
The ADP1173 power switch does not saturate in positive-to-  
negative mode. The voltage drop across the switch can be  
modeled as a 0.75 V base-emitter diode in series with a 0.65 Ω  
resistor. When the switch turns on, inductor current will rise at  
a rate determined by:  
_R't  
L
VL  
R'  
IL (t)=  
1– e  
(9)  
where R' = 0.65 + RL(DC)  
where VL = VIN – 0.75 V  
The effects of capacitor selection on output ripple are demon-  
strated in Figures 11, 12, and 13. These figures show the output  
of the same ADP1173 converter, which was evaluated with  
three different output capacitors. In each case, the peak switch  
current is 500 mA and the capacitor value is 100 µF. Figure 11  
shows a Panasonic HF-series* radial aluminum electrolytic.  
When the switch turns off, the output voltage jumps by about  
90 mV and then decays as the inductor discharges into the  
capacitor. The rise in voltage indicates an ESR of about  
0.18 . In Figure 12, the aluminum electrolytic has been  
replaced by a Sprague 593D-series* tantalum device. In this  
case the output jumps about 35 mV, which indicates an ESR of  
0.07 . Figure 13 shows an OS-CON SA series capacitor in the  
same circuit, and ESR is only 0.02 .  
For example, assume that a –5 V output at 50 mA is to be  
generated from a +4.5 V to +5.5 V source. The power in the  
inductor is calculated from Equation 8:  
PL = |5V|+ 0.5V ×(50 mA)= 275 mW  
(
)
During each switching cycle, the inductor must supply the  
following energy:  
PL 275 mW  
=
=11.5µJ  
fOSC 24 kHz  
*All trademarks are properties of their respective holders.  
REV. 0  
–7–  
ADP1173  
DIODE SELECTION  
In specifying a diode, consideration must be given to speed,  
forward voltage drop and reverse leakage current. When the  
ADP1173 switch turns off, the diode must turn on rapidly if  
high efficiency is to be maintained. Schottky rectifiers, as well as  
fast signal diodes such as the 1N4148, are appropriate. The  
forward voltage of the diode represents power that is not deliv-  
ered to the load, so VF must also be minimized. Again, Schottky  
diodes are recommended. Leakage current is especially impor-  
tant in low current applications, where the leakage can be a  
significant percentage of the total quiescent current.  
For most circuits, the 1N5818 is a suitable companion to the  
ADP1173. This diode has a VF of 0.5 V at 1 A, 4 µA to 10 µA  
leakage, and fast turn-on and turn-off times. A surface mount  
version, the MBRS130T3, is also available. For applications  
where the ADP1173 is “off” most of the time, such as when the  
load is intermittent, a silicon diode may provide higher overall  
efficiency due to lower leakage. For example, the 1N4933 has a  
1 A capability, but with a leakage current of less than 1 µA. The  
higher forward voltage of the 1N4933 reduces efficiency when  
the ADP1173 delivers power, but the lower leakage may outweigh  
the reduction in efficiency.  
Figure 11. Aluminum Electrolytic  
Figure 12. Tantalum Electrolytic  
Figure 13. OS-CON Capacitor  
For switch currents of 100 mA or less, a Schottky diode such as  
the BAT85 provides a VF of 0.8 V at 100 mA and leakage less  
than 1 µA. A similar device, the BAT54, is available in a SOT23  
package. Even lower leakage, in the 1 nA to 5 nA range, can be  
obtained with a 1N4148 signal diode.  
General purpose rectifiers, such as the 1N4001, are not suitable  
for ADP1173 circuits. These devices, which have turn-on times  
of 10 µs or more, are too slow for switching power supply  
applications. Using such a diode “just to get started” will result  
in wasted time and effort. Even if an ADP1173 circuit appears  
to function with a 1N4001, the resulting performance will not  
be indicative of the circuit performance when the correct diode  
is used.  
CIRCUIT OPERATION, STEP-UP (BOOST) MODE  
In boost mode, the ADP1173 produces an output voltage that  
is higher than the input voltage. For example, +12 V can be  
generated from a +5 V logic power supply or +5 V can be  
derived from two alkaline cells (+3 V).  
Figure 16 shows an ADP1173 configured for step-up operation.  
The collector of the internal power switch is connected to the  
output side of the inductor, while the emitter is connected to  
GND. When the switch turns on, pin SW1 is pulled near ground.  
This action forces a voltage across L1 equal to VIN–VCE(SAT),  
and current begins to flow through L1. This current reaches a  
final value (ignoring second-order effects) of:  
If low output ripple is important, the user should consider the  
ADP3000. This device switches at 400 kHz, and the higher  
switching frequency simplifies the design of the output filter.  
Consult the ADP3000 data sheet for additional details.  
All potential current paths must be considered when analyzing  
very low power applications, and this includes capacitor leakage  
current. OS-CON capacitors have leakage in the 5 µA to 10 µA  
range, which will reduce efficiency when the load is also in the  
microampere range. Tantalum capacitors, with typical leakage  
in the 1 µA to 5 µA range, are recommended for very low power  
applications.  
VIN V  
IPEAK  
CE(SAT ) ×23 µs  
L
where 23 µs is the ADP1173 switch’s “on” time.  
REV. 0  
–8–  
ADP1173  
L1  
D1  
When the switch turns off, the magnetic field collapses. The  
polarity across the inductor changes and the switch side of the  
inductor is driven below ground. Schottky diode D1 then turns  
on and current flows into the load. Notice that the Absolute  
Maximum Rating for the ADP1173’s SW2 pin is 0.5 V below  
ground. To avoid exceeding this limit, D1 must be a Schottky  
diode. Using a silicon diode in this application will generate  
forward voltages above 0.5 V, which will cause potentially  
damaging power dissipation within the ADP1173.  
V
V
OUT  
IN  
R3*  
R1  
R2  
2
1
I
V
IN  
LIM  
3
8
SW1  
+
C1  
ADP1173  
FB  
GND SW2  
4
5
* = OPTIONAL  
The output voltage of the buck regulator is fed back to the  
ADP1173’s FB pin by resistors R1 and R2. When the voltage at  
pin FB falls below 1.245 V, the internal power switch turns  
“on” again and the cycle repeats. The output voltage is set by  
the formula:  
Figure 14. Step-Up Mode Operation  
When the switch turns off, the magnetic field collapses. The  
polarity across the inductor changes, current begins to flow  
through D1 into the load and the output voltage is driven above  
the input voltage.  
R1  
VOUT =1.245 V × 1+  
R2  
The output voltage is fed back to the ADP1173 via resistors R1  
and R2. When the voltage at pin FB falls below 1.245 V, SW1  
turns “on” again and the cycle repeats. The output voltage is  
therefore set by the formula:  
When operating the ADP1173 in step-down mode, the output  
voltage is impressed across the internal power switch’s emitter-  
base junction when the switch is off. To protect the switch, the  
output voltage should be limited to 6.2 V or less. If a higher  
output voltage is required, a Schottky diode should be placed in  
series with SW2, as shown in Figure 16.  
R1  
VOUT =1.245 V × 1+  
R2  
If high output current is required in a step-down converter, the  
ADP1111 or ADP3000 should be considered. These devices  
offer higher frequency operation, which reduces inductor size,  
and an external pass transistor can be added to reduce RON of  
the switch.  
The circuit of Figure 14 shows a direct current path from VIN to  
V
OUT, via the inductor and D1. Therefore, the boost converter  
is not protected if the output is short circuited to ground.  
V
CIRCUIT OPERATION, STEP-DOWN (BUCK) MODE  
The ADP1173’s step-down mode is used to produce an output  
voltage lower than the input voltage. For example, the output of  
four NiCd cells (+4.8 V) can be converted to a +3.3 V logic  
supply.  
IN  
R
LIM  
100  
+
2
3
1
C2  
I
V
SW1  
LIM  
IN  
8
4
FB  
L1  
ADP1173  
1N5818  
SW2  
V
OUT  
A typical configuration for step-down operation of the ADP1173  
is shown in Figure 15. In this case, the collector of the internal  
power switch is connected to VIN and the emitter drives the  
inductor. When the switch turns on, SW2 is pulled up toward  
GND  
5
+
R1  
R2  
C1  
D1  
1N5818  
VIN. This forces a voltage across L1 equal to (VIN–VCE) – VOUT  
and causes current to flow in L1. This current reaches a final  
value of:  
,
Figure 16. Step-Down Mode, VOUT > 6.2 V  
VIN VCE VOUT  
If the input voltage to the ADP1173 varies over a wide range, a  
current limiting resistor at Pin 1 may be required. If a particular  
circuit requires high peak inductor current with minimum input  
supply voltage, the peak current may exceed the switch maxi-  
mum rating and/or saturate the inductor when the supply  
voltage is at the maximum value. See the Limiting the Switch  
Current section of this data sheet for specific recommendations.  
IPEAK  
×23 µs  
L
where 23 µs is the ADP1173 switch’s “on” time.  
V
IN  
R3  
100Ω  
+
2
1
3
C2  
I
V
SW1  
LIM  
IN  
8
4
FB  
POSITIVE-TO-NEGATIVE CONVERSION  
L1  
ADP1173  
The ADP1173 can convert a positive input voltage to a negative  
output voltage, as shown in Figure 17. This circuit is essentially  
identical to the step-down application of Figure 15, except that  
the “output” side of the inductor is connected to power ground.  
When the ADP1173’s internal power switch turns off, current  
flowing in the inductor forces the output (–VOUT) to a negative  
potential. The ADP1173 will continue to turn the switch on  
SW2  
V
OUT  
GND  
5
+
R1  
R2  
C1  
D1  
1N5818  
Figure 15. Step-Down Mode Operation  
REV. 0  
–9–  
ADP1173  
until its FB pin is 1.245 V above its GND pin, so the output  
voltage is determined by the formula:  
LIMITING THE SWITCH CURRENT  
The ADP1173’s RLIM pin permits the switch current to be lim-  
ited with a single resistor. This current limiting action occurs on  
a pulse by pulse basis. This feature allows the input voltage to  
vary over a wide range, without saturating the inductor or ex-  
ceeding the maximum switch rating. For example, a particular  
design may require peak switch current of 800 mA with a 2.0 V  
input. If VIN rises to 4 V, however, the switch current will exceed  
1.6 A. The ADP1173 limits switch current to 1.5 A and thereby  
protects the switch, but increases the output ripple. Selecting  
the proper resistor will limit the switch current to 800 mA, even  
if VIN increases. The relationship between RLIM and maximum  
switch current is shown in Figures 4 and 5.  
R1  
VOUT =1.245 V × 1+  
R2  
+V  
IN  
R3  
+
2
3
1
C2  
I
V
SW1  
LIM  
IN  
8
4
FB  
L1  
ADP1173  
SW2  
GND  
5
+
R1  
R2  
C1  
D1  
1N5818  
The ILIM feature is also valuable for controlling inductor current  
when the ADP1173 goes into continuous-conduction mode. This  
occurs in the step-up mode when the following condition is met:  
–V  
OUT  
Figure 17. A Positive-to-Negative Converter  
VOUT +VDIODE  
VIN VSW  
1
<
1– DC  
The design criteria for the step-down application also apply to  
the positive-to-negative converter. The output voltage should be  
limited to |6.2 V|, unless a diode is inserted in series with the  
SW2 Pin (see Figure 16). Also, D1 must again be a Schottky  
diode to prevent excessive power dissipation in the ADP1173.  
where DC is the ADP1173’s duty cycle. When this relationship  
exists, the inductor current does not go all the way to zero dur-  
ing the time the switch is OFF. When the switch turns on for  
the next cycle, the inductor current begins to ramp up from the  
residual level. If the switch ON time remains constant, the in-  
ductor current will increase to a high level (see Figure 19). This  
increases output ripple, and can require a larger inductor and  
capacitor. By controlling switch current with the ILIM resistor,  
output ripple current can be maintained at the design values.  
Figure 20 illustrates the action of the ILIM circuit.  
NEGATIVE-TO-POSITIVE CONVERSION  
The circuit of Figure 18 converts a negative input voltage to a  
positive output voltage. Operation of this circuit configuration is  
similar to the step-up topology of Figure 14, except that the current  
through feedback resistor R1 is level-shifted below ground by a  
PNP transistor. The voltage across R1 is (VOUT–VBEQ1). How-  
ever, diode D2 level-shifts the base of Q1 about 0.6 V below  
ground, thereby cancelling the VBE of Q1. The addition of D2  
also reduces the circuit’s output voltage sensitivity to tempera-  
ture, which otherwise would be dominated by the –2 mV/°C VBE  
contribution of Q1. The output voltage for this circuit is deter-  
mined by the formula:  
R1  
R2  
VOUT = 1.245 V ×  
Unlike the positive step-up converter, the negative-to-positive  
converter’s output voltage can be either higher or lower than the  
input voltage.  
1N5818  
D1  
L1  
Figure 19. (ILIM Operation, RLIM = 0 )  
POSITIVE  
OUTPUT  
+
R
LIM  
C
R1  
Q1  
L
1N4148  
2
1
D2  
+
I
V
IN  
C2  
LIM  
2N3906  
3
8
SW1  
ADP1173  
10kΩ  
FB  
AO SET GND SW2  
4
6
5
7
R2  
NC NC  
NEGATIVE  
INPUT  
Figure 18. A Negative-to-Positive Converter  
Figure 20. (ILIM Operation, RLIM = 240 )  
REV. 0  
–10–  
ADP1173  
+5V  
The internal structure of the ILIM circuit is shown in Figure 21.  
Q1 is the ADP1173’s internal power switch, which is paralleled  
by sense transistor Q2. The relative sizes of Q1 and Q2 are  
scaled so that IQ2 is 0.5% of IQ1. Current flows to Q2 through an  
internal 80 resistor and through the RLIM resistor. These two  
resistors parallel the base-emitter junction of the oscillator-  
disable transistor, Q3. When the voltage across R1 and RLIM  
exceeds 0.6 V, Q3 turns on and terminates the output pulse. If  
only the 80 internal resistor is used (i.e., the ILIM pin is con-  
nected directly to VIN), the maximum switch current will be  
1.5 A. Figures 4 and 5 gives RLIM values for lower current-limit  
values.  
2
ADP1173  
1.245V  
100k  
V
IN  
R1  
R2  
AO  
TO  
PROCESSOR  
REF  
6
V
SET  
BAT  
7
GND  
5
V
–1.245V  
LB  
12.5µA  
= BATTERY TRIP POINT  
R1 =  
V
LB  
R2 = 100kΩ  
Figure 22. Setting the Low Battery Detector Trip Point  
Figure 22 shows the gain block configured as a low battery  
monitor. Resistors R1 and R2 should be set to high values to  
reduce quiescent current, but not so high that bias current in the  
SET input causes large errors. A value of 100 kfor R2 is a  
good compromise. The value for R1 is then calculated from the  
formula:  
I
LIM  
R
LIM  
(EXTERNAL)  
V
IN  
80Ω  
(INTERNAL)  
R1  
SW1  
Q1  
Q3  
VLOBATT 1.245V  
R1=  
DRIVER  
1.245V  
Q2  
OSCILLATOR  
R2  
SW2  
where VLOBATT is the desired low battery trip point. Since the  
gain block output is an open-collector NPN, a pull-up resistor  
should be connected to the positive logic power supply.  
Figure 21. Current Limit Operation  
The delay through the current limiting circuit is approximately  
2 µs. If the switch ON time is reduced to less than 4 µs, accu-  
racy of the current trip-point is reduced. Attempting to program  
a switch ON time of 2 µs or less will produce spurious responses  
in the switch ON time. However, the ADP1173 will still provide  
a properly regulated output voltage.  
5V  
2
ADP1173  
1.245mV  
47kΩ  
V
IN  
R1  
R2  
AO  
TO  
PROCESSOR  
REF  
6
V
SET  
BAT  
7
GND  
5
PROGRAMMING THE GAIN BLOCK  
R3  
The gain block of the ADP1173 can be used as a low-battery  
detector, error amplifier or linear post regulator. The gain block  
consists of an op amp with PNP inputs and an open-collector  
NPN output. The inverting input is internally connected to the  
ADP1173’s 1.245 V reference, while the noninverting input is  
available at the SET pin. The NPN output transistor will sink  
about 100 µA.  
1.6MΩ  
Figure 23. Adding Hysteresis to the Low Battery Detector  
REV. 0  
–11–  
ADP1173  
Typical Circuit Applications  
L1*  
68µH  
100Ω  
1N4148  
2
1
R1  
100Ω  
I
V
IN  
LIM  
3
8
SW1  
9V  
BATTERY  
2.21MΩ  
2
1
ADP1173-5  
1%  
I
V
IN  
LIM  
3
8
SENSE  
SW1  
2 x 1.5V  
CELLS  
GND SW2  
0.1µF  
L1*  
47µH  
ADP1173  
4.7µF  
4
5
5V OUTPUT  
FB  
150mA AT 9V INPUT  
50mA AT 6.5V INPUT  
GND SW2  
118kΩ  
1%  
+
4
5
1N5818  
100µF  
1N5818  
1N5818  
*L1 = GOWANDA GA10-472K  
COILTRONICS CTX50-1  
FOR HIGHER OUTPUT CURRENTS SEE ADP1073 DATASHEET  
22µF  
220kΩ  
*L1 = GOWANDA GA10-682K  
COILTRONICS CTX68-4  
FOR 5V INPUT CHANGE R1 TO 47Ω  
CONVERTER WILL DELIVER –22V AT 40mA  
–22V OUTPUT  
7mA AT 2.0V INPUT  
70% EFFICIENCY  
Figure 27. 9 V to 5 V Converter  
Figure 24. 3 V–22 V LCD Bias Generator  
+V  
IN  
12V-28V  
100Ω  
L1*  
82µH  
2
1
I
V
IN  
LIM  
3
8
SW1  
2
1
ADP1173-5  
I
V
IN  
SENSE  
LIM  
3
8
SW1  
2 x 1.5V  
CELLS  
GND SW2  
L1*  
220µH  
1N5818  
100µF  
ADP1173-5  
4
5
5V OUTPUT  
150mA AT 3V INPUT  
60mA AT 2V INPUT  
SENSE  
5V OUTPUT  
300mA  
GND SW2  
+
+
1N5818  
4
5
100µF  
*L1 = GOWANDA GA10-223K  
*L1 = GOWANDA GA10-822K  
Figure 28. +20 V to 5 V Step-Down Converter  
Figure 25. 3 V to 5 V Step-Up Converter  
+V  
IN  
5V INPUT  
+
22µF  
100Ω  
2
1
I
V
IN  
LIM  
3
8
SW1  
ADP1173-5  
SENSE  
GND  
5
SW2  
L1*  
100µH  
4
+
100µF  
1N5818  
–5V OUTPUT  
75mA  
*L1 = GOWANDA GA10-103K  
COILTRONICS CTX100-1  
Figure 26. +5 V to –5 V Converter  
REV. 0  
–12–  
ADP1173  
L1*  
500µH  
MUR110  
44mH  
44mH  
+5V  
100mA  
~
~
+
+
47µF  
100V  
48V DC  
+
390kΩ  
220µF  
10V  
3.6MΩ  
10kΩ  
2N5400  
VN2222L  
12V  
IRF530  
15V  
10nF  
*L1 = CTX110077  
= 120µA  
100Ω  
I
Q
1N4148  
2
1
I
V
IN  
LIM  
3
8
SW1  
10µF  
16V  
+
ADP1173  
1N965B  
FB  
GND SW2  
4
5
110kΩ  
Figure 29. Telecom Supply  
L1*  
100µH  
1N5818  
SI9405DY  
V
= 5V AT 100mA  
OUT  
AT V = 2.6V  
IN  
56Ω  
470kΩ  
+
2
1
75k  
470µF  
I
V
3
LIM  
IN SW1  
4 x NICAD  
OR  
ALKALINE  
CELLS  
7
SETADP1173  
+
6
8
AO  
470µF  
FB  
GND SW2  
+
4
5
240Ω  
24kΩ  
470µF  
*L1 = GOWANDA GA20-103K  
COILTRONICS CTX100-4  
V
= 2.6V TO 7.2V  
IN  
Figure 30. 5 V to 5 V Step-Up or Step-Down Converter  
L1*  
20µH, 5A  
1N5820  
100kΩ  
47kΩ  
220Ω  
2
1
100kΩ  
2.2MΩ  
100Ω  
I
V
IN  
LIM  
6
+
2N3906  
AO  
3
8
2N4403  
SW1  
FB  
470µF  
ADP1173  
+5V OUTPUT  
200mA  
LOCKOUT AT  
1.85V INPUT  
301kΩ  
7
SET  
GND  
2 x NICAD  
SW2  
4
5
5Ω  
+
470µF  
100kΩ  
MJE200  
47Ω  
100kΩ  
*L1 = COILTRONICS CTX-20-5-52  
1% METAL FILM  
Figure 31. 2 V to 5 V at 200 mA Step-Up Converter with Undervoltage Lockout  
REV. 0  
–13–  
ADP1173  
L1*  
25µH, 2A  
0.22Ω  
MTM20P08  
V
IN  
7V-24V  
18V  
1W  
1N5820  
1N5818  
2kΩ  
+
2N3904  
51Ω  
470µF  
2
1
I
V
IN  
LIM  
3
SW1  
100Ω  
1/2W  
1N4148  
–V  
V
= –5.13*V  
C
OUT  
V
IN  
ADP1173  
200kΩ  
39kΩ  
(0V TO +5V)  
C
8
FB  
OP196  
*L1 = GOWANDA GT10-100  
SW2  
4
GND  
5
EFFICIENCY 80% FOR 10mA I  
500mA  
LOAD  
STANDBY I 150µA  
Q
Figure 32. Voltage Controlled Positive-to-Negative Converter  
L1*  
25µH, 2A  
0.22Ω  
MTM20P08  
V
5V  
500mA  
IN  
7V-24V  
+
18V  
1W  
1N5820  
1N5818  
2kΩ  
470µF  
2N3904  
51Ω  
2
1
I
V
IN  
LIM  
3
SW1  
100Ω  
1/2W  
1N4148  
ADP1173  
121kΩ  
FB  
8
GND SW2  
40.2kΩ  
4
5
*L1 = GOWANDA GT10-100  
EFFICIENCY 80% FOR 10mA I  
500mA  
LOAD  
OPERATE STANDBY  
STANDBY I 150µA  
Q
Figure 33. High Power, Low Quiescent Current Step-Down Converter  
REV. 0  
–14–  
ADP1173  
OUTLINE DIMENSIONS  
Dimensions shown in inches and (mm).  
8-Lead Plastic DIP  
(N-8)  
0.430 (10.92)  
0.348 (8.84)  
8
5
4
0.280 (7.11)  
0.240 (6.10)  
1
0.325 (8.25)  
0.300 (7.62)  
0.060 (1.52)  
0.015 (0.38)  
PIN 1  
0.195 (4.95)  
0.115 (2.93)  
0.210 (5.33)  
MAX  
0.130  
(3.30)  
MIN  
0.160 (4.06)  
0.115 (2.93)  
0.015 (0.381)  
0.008 (0.204)  
SEATING  
PLANE  
0.100  
(2.54)  
BSC  
0.022 (0.558)  
0.014 (0.356)  
0.070 (1.77)  
0.045 (1.15)  
8-Lead Small Outline Package  
(SO-8)  
0.1968 (5.00)  
0.1890 (4.80)  
8
1
5
4
0.1574 (4.00)  
0.1497 (3.80)  
0.2440 (6.20)  
0.2284 (5.80)  
PIN 1  
0.0688 (1.75)  
0.0532 (1.35)  
0.0196 (0.50)  
0.0099 (0.25)  
x 45°  
0.0098 (0.25)  
0.0040 (0.10)  
8°  
0°  
0.0500  
(1.27)  
BSC  
0.0192 (0.49)  
0.0138 (0.35)  
SEATING  
PLANE  
0.0098 (0.25)  
0.0075 (0.19)  
0.0500 (1.27)  
0.0160 (0.41)  
REV. 0  
–15–  
–16–  

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