AD ADP1109AR-5

a
Micropower Low Cost
Fixed 3.3 V, 5 V, 12 V and Adjustable
DC-to-DC Converter
ADP1109
FEATURES
Operates at Supply Voltages 2 V to 12 V
Fixed 3.3 V, 5 V, 12 V and Adjustable Output
Minimum External Components Required
Ground Current: 320 mA
Oscillator Frequency: 120 kHz
Logic Shutdown
8-Lead DIP and SO-8 Packages
FUNCTIONAL BLOCK DIAGRAMS
VIN
SENSE
ADP1109-3.3: R1 = 152kV
ADP1109-5: R1 = 83kV
ADP1109-12: R1 = 29kV
R2
250kV
SW
COMPARATOR
1.25V
REFERENCE
APPLICATIONS
Cellular Telephones
Single-Cell to 5 V Converters
Laptop and Palmtop Computers
Pagers
Cameras
Battery Backup Supplies
Portable Instruments
Laser Diode Drivers
Hand-Held Inventory Computers
+
A1
120kHz
OSCILLATOR
Q1
DRIVER
R1
SHUTDOWN
GND
Fixed Output
VIN
FB
ADP1109
SW
COMPARATOR
1.25V
REFERENCE
+
A1
120kHz
OSCILLATOR
GENERAL DESCRIPTION
Q1
DRIVER
The ADP1109 is a versatile step-up switching regulator. The
device requires only minimal external components to operate as
a complete switching regulator.
SHUTDOWN
GND
Adjustable Output
The ADP1109-5 can deliver 100 mA at 5 V from a 3 V input
and the ADP1109-12 can deliver 60 mA at 12 V from a 5 V
input. The device also features a logic controlled shutdown
capability that, when a logic low is applied, will shut down the
oscillator.
TYPICAL APPLICATION
The 120 kHz operating frequency allows for the use of small
surface mount components. The gated oscillator capability
eliminates the need for frequency compensation.
L1
33mH
VIN
5V
VIN
D1
SW
SENSE
ADP1109-12
SHUTDOWN
GND
+ C1
22mF
16V
VOUT
12V
60mA
SHUTDOWN/PROGRAM
Flash Memory VPP Generator
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: 781/329-4700
World Wide Web Site: http://www.analog.com
Fax: 781/326-8703
© Analog Devices, Inc., 1998
ADP1109–SPECIFICATIONS (08C ≤ T ≤ +708C, V
A
IN
= 3 V unless otherwise noted)
Parameter
Conditions
Symbol
QUIESCENT CURRENT
Switch Off
IQ
INPUT VOLTAGE
VIN
COMPARATOR TRIP POINT
VOLTAGE
Min
ADP1109
OUTPUT VOLTAGE
ADP1109-3.3
ADP1109-5
ADP1109-12
2 V ≤ VIN ≤ 3 V
3 V ≤ VIN ≤ 5 V
3 V ≤ VIN ≤ 12 V
VOUT
Max
Units
450
590
µA
9
V
1.25
1.30
V
8
14
mV
3.30
5.00
12.00
3.46
5.25
12.55
V
V
V
16
20
40
40
50
110
mV
mV
mV
2
1.20
COMPARATOR HYSTERESIS
Typ
3.13
4.75
11.45
OUTPUT VOLTAGE RIPPLE
ADP1109-3.3
ADP1109-5
ADP1109-12
OSCILLATOR FREQUENCY
TA = +25°C
fOSC
100
90
120
140
155
kHz
kHz
DUTY CYCLE
Full Load
DC
40
50
70
%
SWITCH-ON TIME
TA = +25°C
tON
3.1
3.0
4.2
5.9
6.5
µs
µs
SWITCH SATURATION VOLTAGE
ADP1109-3.3
ADP1109-5
ADP1109-12
ISW = 500 mA
VIN = 3 V
VIN = 3 V
VIN = 5 V
VCESAT
0.4
0.4
0.4
0.8
0.8
0.8
V
V
V
SWITCH LEAKAGE CURRENT
VSW = 12 V, TA = +25°C
1
10
µA
SHUTDOWN PIN HIGH
VIH
2.0
V
SHUTDOWN PIN LOW
VIL
0.8
V
SHUTDOWN PIN INPUT CURRENT
VSHUTDOWN = 2 V
IIH
10
µA
SHUTDOWN PIN INPUT CURRENT
VSHUTDOWN = 0.8 V
IIL
20
µA
NOTES
All limits at temperature extremes are guaranteed via correlation using standard quality control methods.
Specifications subject to change without notice.
L1 = CTX15-1
L1
15mH
L1 = CTX15-1
L1
15mH
1N5818
+5V
VIN = 2V
SW
VIN
ADP1109-5
+12V
SW
VIN
+ 22mF
16V
GND
1N5818
VIN = 2V
300mA
at 3V INPUT
50mA
at 2V INPUT
SENSE
L1 = CTX15-1
L1
15mH
40mA
at 3V INPUT
10mA
at 2V INPUT
SENSE
ADP1109-12
1N5818
+5V
VIN = 2V
SW
VIN
SENSE
ADP1109-12
+ 10mF
20V
300mA
at 3V INPUT
50mA
at 2V INPUT
+ 22mF
16V
SHUTDOWN
GND
GND
SHUTDOWN
Figure 1. 2 V to 5 V Converter
Figure 2. 2 V to 12 V Converter
–2–
Figure 3. 2 V to 5 V Converter
With Shutdown
REV. 0
ADP1109
ABSOLUTE MAXIMUM RATINGS*
PIN CONFIGURATIONS
Supply Voltage, VOUT . . . . . . . . . . . . . . . . . . . . –0.4 V to 20 V
SW Pin Voltage . . . . . . . . . . . . . . . . . . . . . . . . –0.4 V to 50 V
Shutdown Pin Voltage . . . . . . . . . . . . . . . . . . . . . . . . . . 6.0 V
Switch Current . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 1.2 A
Maximum Power Dissipation . . . . . . . . . . . . . . . . . . 300 mW
Operating Temperature Range . . . . . . . . . . . . 0°C to +70°C
Storage Temperature Range . . . . . . . . . . . . –65°C to +150°C
Lead Temperature (Soldering, 10 sec) . . . . . . . . . . . +300°C
8-Lead Plastic DIP
(N-8)
8
VIN 1
ADP1109A
FB(SENSE)*
SHUTDOWN
TOP VIEW
SW 3 (Not to Scale) 6 NC
NC 2
*This is a stress rating only; operation beyond these limits can cause the device to
be permanently damaged.
GND 4
7
5
NC
NC = NO CONNECT
*FIXED VERSIONS
ORDERING GUIDE
Model
Output
Voltage
Package
Description
Package
Options
ADP1109AN
ADP1109AR
ADP1109AN-3.3
ADP1109AR-3.3
ADP1109AN-5
ADP1109AR-5
ADP1109AN-12
ADP1109AR-12
ADJ
ADJ
3.3 V
3.3 V
5V
5V
12 V
12 V
Plastic DIP
Small Outline IC
Plastic DIP
Small Outline IC
Plastic DIP
Small Outline IC
Plastic DIP
Small Outline IC
N-8
SO-8
N-8
SO-8
N-8
SO-8
N-8
SO-8
8-Lead SOIC
(SO-8)
VIN 1
8
FB(SENSE)*
NC 2 ADP1109A 7 SHUTDOWN
TOP VIEW
SW 3 (Not to Scale) 6 NC
GND 4
5
NC
NC = NO CONNECT
*FIXED VERSIONS
PIN FUNCTION DESCRIPTIONS
Pin
Mnemonic
Function
1
2, 5, 6
3
4
7
VIN
NC
SW
GND
SHUTDOWN
8
FB(SENSE)
Input Supply Voltage.
No Connection.
Collector Node of Power Transistor.
Ground.
When logic low is applied to this pin,
oscillator is shut down.
On the ADP1109A (Adjustable), this
pin goes directly to the comparator
input. On the ADP1109-3.3,
ADP1109-5 and ADP1109-12, this
pin is connected through the internal
resistor that sets the output voltage.
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 ADP1109 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.
REV. 0
–3–
WARNING!
ESD SENSITIVE DEVICE
ADP1109 –Typical Performance Characteristics
1.2
600
1.0
500
122.5
122.0
QUIESCENT CURRENT – mA
123.0
0.8
VCESAT – V
OSCILLATOR FREQUENCY – kHz
123.5
121.5
121.0
120.5
0.6
0.4
120.0
119.5
0.2
400
300
200
100
119.0
118.5
2
4
6
8 10 12 14 16
INPUT VOLTAGE – V
18
0
0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9
SWITCH CURRENT – A
20
Figure 4. Oscillator Frequency vs.
Input Voltage
Figure 5. Switch Saturation Voltage
vs. Switch Current
2
4
6
8
10 12 14 16
INPUT VOLTAGE – V
18
20
Figure 6. Quiescent Current vs.
Input Voltage
4.5
58
4.4
56
4.3
54
130
120
110
100
90
–40
0
25
70
TEMPERATURE – 8C
4.2
4.1
4.0
Figure 7. Oscillator Frequency vs.
Temperature
50
48
46
3.8
44
0
25
70
TEMPERATURE – 8C
85
42
–40
0
25
70
TEMPERATURE – 8C
85
Figure 9. Duty Cycle vs. Temperature
Figure 8. Switch-On Time vs.
Temperature
0.39
52
3.9
3.7
–40
85
DUTY CYCLE – %
140
SWITCH-ON TIME – ms
OSCILLATOR FREQUENCY – kHz
150
0
1
600
QUIESCENT CURRENT – mA
0.38
VCE(SAT) – V
0.37
0.36
0.35
0.34
0.33
0.32
0.31
–40
0
25
70
TEMPERATURE – 8C
85
Figure 10. Switch Saturation Voltage
vs. Temperature
500
400
300
200
100
0
–40
0
25
70
TEMPERATURE – 8C
85
Figure 11. Quiescent Current vs.
Temperature
–4–
REV. 0
ADP1109
The ADP1109 is designed for applications where the input
voltage is fairly stable, such as generating +12 V from a +5 V
logic supply. The ADP1109 does not have an internal switch
current limiting circuit, so the inductor may saturate if the input
voltage is too high. The ADP1111 or ADP3000 should be
considered for battery powered and similar applications where
the input voltage varies.
APPLICATION INFORMATION
THEORY OF OPERATION
The ADP1109 is a flexible, low power switch-mode power supply (SMPS) controller for step-up dc/dc converter applications.
This device uses a gated-oscillator technique to provide very
high performance with low quiescent current. For example,
more than 2 W of output power can be generated from a +5 V
source, while quiescent current is only 450 µA.
A functional block diagram of the ADP1109 is shown on page 1.
The internal 1.25 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 1.25 V, the
120 kHz oscillator turns on. A driver amplifier provides base
drive to the internal power switch, and the switching action
raises the output voltage. When the voltage at the FB pin exceeds 1.25 V, the oscillator is shut off. While the oscillator is off,
the ADP1109 quiescent current is only 450 µA. The comparator
includes a small amount of hysteresis, which ensures loop stability without requiring external components for frequency compensation.
A shutdown feature permits the oscillator to be shut off. Holding SHUTDOWN low will disable the oscillator, and the
ADP1109’s quiescent current will remain 450 µA.
Calculating the Inductor Value
Selecting the proper inductor value is a simple, two-step process:
1. Define the operating parameters: minimum input voltage,
maximum input voltage, output voltage and output current.
2. Calculate the inductor value, using the equations in the following section.
Inductor Selection
In a step-up, or boost, converter (Figure 1), the inductor must
store enough power to make up the difference between the input
voltage and the output voltage. The inductor power is calculated
from the equation:
(
) ( )
P L = VOUT +V D −VIN ( MIN ) × IOUT
The output voltage of the ADP1109 is set with two external
resistors. Three fixed-voltage models are also available: the
ADP1109-3.3 (+3.3 V), ADP1109-5 (+5 V) and ADP1109-12
(+12 V). The fixed-voltage models are identical to the ADP1109,
except that laser-trimmed voltage-setting resistors are included on
the chip. On the fixed-voltage models of the ADP1109, simply
connect the SENSE pin (Pin 8) directly to the output voltage.
(1)
where VD is the diode forward voltage (<0.5 V for a 1N5818
Schottky). Energy is stored in the inductor only while the
ADP1109 switch is ON, so the energy stored in the inductor on
each switching cycle must be must be equal to or greater than:
PL
f OSC
COMPONENT SELECTION
General Notes on Inductor Selection
(2)
in order for the ADP1109 to regulate the output voltage. When the
internal power switch turns ON, current flow in the inductor
increases at the rate of:
When the ADP1109 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.
()
IL t =
To specify an inductor for the ADP1109, the proper values of
inductance, saturation current and dc resistance must be determined. This process is not difficult, and specific equations 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 ADP1109 applications, an inductor of 10 µH to 47 µH, with a saturation current rating of
300 mA to 1 A and dc resistance <0.4 Ω is suitable. Ferrite core
inductors that meet these specifications are available in small,
surface-mount packages. Air-core inductors, as well as RF chokes,
are unsuitable because of their low peak current ratings.
REV. 0
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.
−R ' t 
V IN 
L
1−
e

R' 

(3)
where L is in Henrys and R' is the sum of the switch equivalent
resistance (typically 0.8 Ω at +25°C) and the dc resistance of
the inductor. In most applications, the voltage drop across the
switch is small compared to VIN so a simpler equation can be
used:
()
IL t =
V IN
t
L
(4)
Replacing t in the above equation with the ON time of the
ADP1109 (5.5 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:
1
E L = L × I 2 peak
2
–5–
(5)
ADP1109
As previously mentioned, EL must be greater than PL/fOSC so
that the ADP1109 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 possible to minimize losses in the switch, inductor and
diode.
In practice, the inductor value is easily selected using the equations above. For example, consider a supply that will generate
12 V at 120 mA from a +5 V source. The inductor power required is, from Equation 1:
PL = (12 V + 0.5 V – 5 V) × (120 mA) = 900 mW
(6)
(7)
V IN
5V
t=
5.5 µs = 45.8 µH
I L ( MAX )
600 mA
(8)
Substituting a standard inductor value of 33 µH, with 0.2 Ω dc
resistance, will produce a peak switch current of:
I PEAK
5V
=
1.0 Ω
–1.0 Ω × 5.5 µs 

33 µH
1−
e

 = 768 mA


(
) (
1
33 µH × 768 mA
2
)
2
= 9.7 µJ
(11)
For optimum performance, the ADP1109’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 capacitors,
specifically designed for switch mode converter applications, 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.
Diode Selection
(9)
Once the peak current is known, the inductor energy can be
calculated from Equation 5:
EL =

R2 
VOUT = 1.25 V × 1+
R1 

Capacitor Selection
The required inductor power is fairly low in this example, so
the peak current can also be low. Assuming a peak current of
600 mA as a starting point, Equation 4 can be rearranged to
recommend an inductor value:
L=
The output voltage is fed back to the ADP1109 via resistors R1
and R2 (Figure 5). When the voltage at the comparator’s inverting input falls below 1.25 V, the oscillator turns “on” and the
output voltage begins to rise. The output voltage is therefore set
by the formula:
Resistors R1 and R2 are provided internally on fixed-voltage
versions of the ADP1109. In this case, a complete dc-dc converter requires only four external components.
On each switching cycle, the inductor must supply:
P L 900 mW
=
= 7.5 µJ
f OSC 120 kHz
Output Voltage Selection
(10)
The inductor energy of 9.7 µJ is greater than the PL /fOSC requirement of 7.5 µJ, so the 33 µH inductor will work in this
application. By substituting other inductor values into the same
equations, the optimum inductor value can be selected. When
selecting an inductor, the peak current must not exceed the
maximum switch current of 1.2 A. If the calculated peak current
is greater than 1.2 A, either the input voltage must be increased
or the load current decreased.
In specifying a diode, consideration must be given to speed,
forward voltage drop and reverse leakage current. When the
ADP1109 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
delivered to the load, so VF must also be minimized. Again,
Schottky diodes are recommended. Leakage current is especially
important 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
ADP1109. 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 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 an
SOT-23 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 ADP1109 circuits. These devices, which have turn-on times
of 10 µs or more, are far 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 ADP1109 circuit appears
to function with a 1N4001, the resulting performance will not
be indicative of the circuit performance when the correct diode
is used.
–6–
REV. 0
ADP1109
OUTLINE DIMENSIONS
Dimensions shown in inches and (mm).
8-Lead Plastic DIP
(N-8)
0.430 (10.92)
0.348 (8.84)
8
5
0.280 (7.11)
0.240 (6.10)
1
4
0.060 (1.52)
0.015 (0.38)
PIN 1
0.210 (5.33)
MAX
0.325 (8.25)
0.300 (7.62)
0.195 (4.95)
0.115 (2.93)
0.130
(3.30)
MIN
0.160 (4.06)
0.115 (2.93)
0.022 (0.558) 0.100 0.070 (1.77)
0.014 (0.356) (2.54) 0.045 (1.15)
BSC
0.015 (0.381)
0.008 (0.204)
SEATING
PLANE
8-Lead SOIC
(SO-8)
0.1968 (5.00)
0.1890 (4.80)
0.1574 (4.00)
0.1497 (3.80)
PIN 1
0.0098 (0.25)
0.0040 (0.10)
SEATING
PLANE
REV. 0
8
5
1
4
0.2440 (6.20)
0.2284 (5.80)
0.0688 (1.75)
0.0532 (1.35)
0.0500 0.0192 (0.49)
(1.27) 0.0138 (0.35)
BSC
0.0196 (0.50)
x 45°
0.0099 (0.25)
0.0098 (0.25)
0.0075 (0.19)
–7–
8°
0°
0.0500 (1.27)
0.0160 (0.41)
–8–
PRINTED IN U.S.A.
C3251–8–1/98