ETC ADP3050AR-3.3

a
FEATURES
Wide Input Voltage Range: 3.6 V to 30 V
Adjustable and Fixed (3.3 V, 5 V) Output Options
Integrated 1 A Power Switch
Uses Small Surface-Mount Components
Cycle-By-Cycle Current Limiting
Peak Input Voltage (100 ms): 60 V
Thermally Enhanced 8-Lead SOIC Package
Configurable as a Buck, Buck-Boost and SEPIC
Regulator
APPLICATIONS
Industrial Power Systems
PC Peripheral Power Systems
Preregulator for Linear Regulators
Distributed Power Systems
Automotive Systems
Battery Chargers
200 kHz, 1 A High-Voltage
Step-Down Switching Regulator
ADP3050
FUNCTIONAL BLOCK DIAGRAM
BIAS
SD
IN
CURRENT SENSE
AMPLIFIER
2.5V
REGULATOR
GND
FREQUENCY
AND CURRENT LIMIT
FOLDBACK
+
CURRENT
LIMIT
200kHz
OSCILLATOR
BOOST
FB
CMP
S
Q
DRIVER
R
gm
SWITCH
ADP3050
1.2V
COMP
GENERAL DESCRIPTION
The ADP3050 is a current-mode monolithic buck (step-down)
PWM switching regulator that contains a high current 1 A power
switch and all control, logic, and protection functions. It uses a
unique compensation scheme that allows the use of any type of
output capacitor (tantalum, ceramic, electrolytic, OS-CON).
Unlike some buck regulators, the design is not restricted to using
a specific type of output capacitor or ESR value.
A special boosted drive stage is used to saturate the NPN power
switch, providing a system efficiency higher than conventional
bipolar buck switchers. Further efficiency improvements are
obtained by using the low voltage regulated output to provide
the device's internal operating current. A high switching frequency
allows the use of small external surface-mount components. A
wide variety of standard off-the-shelf devices can be used, providing a great deal of design flexibility. A complete regulator
design requires only a few external components.
The ADP3050 includes a shutdown input that places the device
in a low-power mode, reducing the total supply current to under
20 µA. Internal protection features include thermal shutdown
circuitry and a cycle-by-cycle current-limit for the power switch
to provide complete device protection under fault conditions.
The ADP3050 provides excellent line and load regulation,
maintaining typically less than ± 3% output voltage accuracy
over temperature and under all input voltage and output current conditions.
The ADP3050 is specified over the industrial temperature range of
–40°C to +85°C and is available in a thermally enhanced 8-lead
SOIC package.
REV. A
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., 2000
1
ADP3050–SPECIFICATIONS (V
Parameter
FEEDBACK
Feedback Voltage
ADP3050
ADP3050-3.3
ADP3050-5
Line Regulation
Load Regulation
Input Bias Current
ERROR AMPLIFIER
Transconductance2
Voltage Gain2
Output Current
ADP3050
ADP3050-3.3
ADP3050-5
OSCILLATOR
Oscillator Frequency3
Minimum Duty Cycle
Maximum Duty Cycle
SWITCH
Average Output Current Limit4
ADP3050
ADP3050-3.3
ADP3050-5
Peak Switch Current Limit5
Saturation Voltage
Leakage Current
IN
= 10 V, TA = –40ⴗC to +85ⴗC, unless otherwise noted)
Symbol
Conditions
VFB
Over Line and Temperature
IFB
VIN = 10 V to 30 V, no load
ILOAD = 100 mA to 1 A,
ADP3050AR Only
ADP3050AR-3.3, ADP3050AR-5
ADP3050AR Only
Typ
Max
Unit
1.16
3.20
4.85
1.20
3.30
5.00
0.005
1.24
3.40
5.15
V
V
V
%/V
–1.0
–0.5
+0.1
+0.1
0.65
+1.0
+0.5
2
%/A
%/A
µA
gm
AVOL
COMP = 1.0 V, FB = 1.1 V to 1.3 V
COMP = 1.0 V, FB = 3.0 V to 3.6 V
COMP = 1.0 V, FB = 4.5 V to 5.5 V
fOSC
DMIN
DMAX
1250
300
µMho
V/V
± 115
± 120
± 135
µA
µA
µA
170
200
10
90
240
kHz
%
%
1.0
1.0
1.0
1.5
1.25
1.25
1.25
1.7
0.65
50
1.5
1.5
1.5
2.1
0.95
A
A
A
A
V
nA
0.4
V
V
30
3.0
3.0
V
V
V
1.5
40
6.0
mA
µA
mA
mA
mA
ICL(AVG)
BOOST = 15 V, FB = 1.1 V
BOOST = 15 V, FB = 3.0 V
BOOST = 15 V, FB = 4.5 V
ICL(PEAK)
BOOST = 15 V, ILOAD = 1 A
SHUTDOWN
Input Voltage Low
Input Voltage High
SUPPLY
Input Voltage Range6
Minimum BIAS Voltage
Minimum BOOST Voltage
IN Supply Current
Normal Mode
Shutdown Mode
BIAS Supply Current
BOOST Supply Current
Min
2.0
VIN
VBIAS
VBOOST
IQ
IBIAS
IBOOST
3.6
BIAS = 5.0 V
SD = 0 V, VIN ≤ 30 V
BIAS = 5.0 V
BOOST = 15 V, ISW = 0.5 A
BOOST = 15 V, ISW = 1.0 A
0.7
15
4.0
18
20
40
NOTES
1
All limits at temperature extremes are guaranteed via correlation using standard Statistical Quality Control (SQC).
2
Transconductance and voltage gain measurements refer to the internal amplifier without the voltage divider. To calculate the transconductance and gain of the fixed
voltage parts, divide the values shown by FB/1.20.
3
The switching frequency is reduced when the feedback pin is lower than 0.8 ⫻ FB.
4
See Figure 1 for test circuit.
5
Switch current limit is measured with no diode, no inductor, and no output capacitor.
6
Minimum input voltage is not measured directly, but is guaranteed by other tests. The actual minimum input voltage needed to keep the output in regulation will
depend on output voltage and load current.
Specifications subject to change without notice.
–2–
REV. A
ADP3050
ABSOLUTE MAXIMUM RATINGS*
PIN FUNCTION DESCRIPTION
IN Voltage
Continuous . . . . . . . . . . . . . . . . . . . . . . . . –0.3 V to +40 V
Peak (<100 ms) . . . . . . . . . . . . . . . . . . . . . –0.3 V to +60 V
BOOST Voltage
Continuous . . . . . . . . . . . . . . . . . . . . . . . . –0.3 V to +45 V
Peak (<100 ms) . . . . . . . . . . . . . . . . . . . . . –0.3 V to +65 V
SD, BIAS Voltage . . . . . . . . . . . . . . . . . –0.3 V to IN + 0.3 V
FB Voltage . . . . . . . . . . . . . . . . . . . . . . . . . . . . –0.3 V to +8 V
COMP Voltage . . . . . . . . . . . . . . . . . . . –0.3 V to IN + 0.3 V
SWITCH Voltage . . . . . . . . . . . . . . . . . –0.3 V to IN + 0.3 V
Operating Ambient Temperature Range . . . . –40°C to +85°C
Operating Junction Temperature Range . . . –40°C to +125°C
Storage Temperature Range . . . . . . . . . . . . –65°C to +150°C
θJA (2-Layer PCB) . . . . . . . . . . . . . . . . . . . . . . . . . . 108°C/W
θJA (4-Layer PCB) . . . . . . . . . . . . . . . . . . . . . . . . . . . 81°C/W
Lead Temperature Range (Soldering, 60 sec) . . . . . . . . 300°C
Pin Mnemonic Function
1
SWITCH
2
BOOST
3
BIAS
*This is a stress rating only; operation beyond these limits can cause the device to
be permanently damaged. Unless otherwise specified, all voltages are referenced
to GND
4
FB
ORDERING GUIDE
5
COMP
6
SD
7
8
GND
IN
Model
Output
Voltage
Temperature
Range
Package*
ADP3050AR
ADP3050AR-3.3
ADP3050AR-5
ADJ
3.3 V
5.0 V
–40°C to +85°C
–40°C to +85°C
–40°C to +85°C
SO-8
SO-8
SO-8
*SO = Small Outline Package
PIN CONFIGURATION
8-Lead SOIC
(R-Suffix)
SWITCH 1
BOOST 2
8
ADP3050
This is the emitter of the internal NPN
power switch. The voltage at this pin switches
between VIN and approximately –0.5 V.
This pin is used to provide a boosted voltage
(higher than VIN) for the drive stage of the
NPN power switch. With the higher drive
voltage, the power switch can be saturated,
greatly reducing the switch power losses.
Connect this pin to the regulated output
voltage to maximize system efficiency.
When this pin is above 2.7 V, most of the
ADP3050 operating current will be taken
from the output instead of the input supply.
Leave unconnected if not used.
This feedback pin senses the regulated output
voltage. Connect this pin directly to the output (fixed output versions).
This pin is used to compensate the regulator
with an external resistor and capacitor. This
pin can be used to override the control loop,
but the voltage on this pin should not exceed
about 2 V, as the pin is internally clamped to
ensure a fast transient response. Use a pull-up
resistor if this pin is to be pulled higher than 2 V.
Use this pin to turn the device on and off. If
this feature is not needed, tie this pin directly
to VIN.
Connect this pin to local ground plane.
Connect this pin to the input supply voltage.
An input bypass capacitor must be placed
close to this pin to ensure proper regulator
operation.
IN
GND
TOP VIEW
BIAS 3 (Not to Scale) 6 SD
FB 4
5 COMP
7
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 this device 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. A
–3–
ADP3050 – Typical Performance Characteristics
2.0
VIN = 10V, NO LOAD
VIN = 10V
4.5
1.8
4.0
AVERAGE OUTPUT CURRENT – A
QUIESCENT OPERATING CURRENT – mA
5.0
INTO BIAS PIN
3.5
3.0
2.5
2.0
1.5
1.0
INTO VIN PIN
0.5
0
ⴚ45 ⴚ35 ⴚ25 ⴚ15 ⴚ5
1.4
1.2
1.0
0.8
0.6
0.4
0.2
5 15 25 35 45
TEMPERATURE – ⴗC
55
65
75
0
ⴚ45 ⴚ35 ⴚ25 ⴚ15 ⴚ5
85
TPC 1. Quiescent Operating Current vs. Temperature
55
65
75
85
25
VIN = 10V
20
BOOST CURRENT – mA
20
15
10
15
10
5
5
0
0
0
5
10
15
20
SUPPLY VOLTAGE – V
25
0
30
TPC 2. Shutdown Quiescent Current vs. Supply Voltage
0.1
0.2
0.3
0.4
0.5
0.6
0.7
LOAD CURRENT – A
0.8
0.9
1.0
TPC 5. Boost Current vs. Load Current
100
10
BIAS TIED TO VOUT
VIN = 6V
90
80
8
70
EFFICIENCY – %
QUIESCENT OPERATING CURRENT – mA
5
15 25 35 45
TEMPERATURE – ⴗC
TPC 4. Average Output Current Limit vs. Temperature
25
SHUTDOWN QUIESCENT CURRENT – ␮A
1.6
6
VOUT = 5V
4
VOUT = 3.3V
VIN = 24V
VIN = 12V
60
VIN = 18V
VIN = 30V
50
L = 33␮H
CIN = 22␮F
COUT = 100␮F
40
30
20
2
10
0
0
0
5
10
15
20
SUPPLY VOLTAGE – V
25
30
0
200
400
600
800
1k
OUTPUT CURRENT – mA
TPC 3. Quiescent Operating Current vs. Supply Voltage
TPC 6. 5 V Output Efficiency
–4–
REV. A
ADP3050
0.6
100
VOUT = 3.3V
VIN = 5V
OUTPUT VOLTAGE CHANGE – %
90
80
EFFICIENCY – %
70
60
VIN = 12V
VIN = 24V
VIN = 30V
VIN = 18V
50
40
L = 33␮H
CIN = 22␮F
COUT = 100␮F
30
20
0.4
0.2
ILOAD = 100mA
0
ILOAD = 1A
ⴚ0.2
ⴚ0.4
10
0
0
200
400
600
800
ⴚ0.6
1k
0
10
20
INPUT VOLTAGE – V
OUTPUT CURRENT – mA
TPC 7. 3.3 V Output Efficiency
TPC 10. 3.3 V Output Voltage Change vs. Input Voltage
8
0.5
VIN = 10V
ILOAD = 1A
0.4
7
0.3
MINIMUM INPUT VOLTAGE – V
OUTPUT VOLTAGE CHANGE – %
30
0.2
0.1
0
ⴚ0.1
ⴚ0.2
ⴚ0.3
VOUT = 5V
6
5
4
VOUT = 3.3V
3
ⴚ0.4
ⴚ0.5
ⴚ45 ⴚ35 ⴚ25 ⴚ15 ⴚ5
5 15 25 35 45
TEMPERATURE – ⴗC
55
65
75
2
0
85
TPC 8. Output Voltage Change vs. Temperature
0.2
0.3
0.4
0.5
0.6 0.7
LOAD CURRENT – A
0.8
0.9
1.0
TPC 11. Minimum Input Voltage vs. Load Current
0
0.6
VIN = 10V
VOUT = 5V
ⴚ0.02
0.4
OUTPUT VOLTAGE CHANGE – %
OUTPUT VOLTAGE CHANGE – %
0.1
0.2
ILOAD = 1A
0.0
ILOAD = 100mA
ⴚ0.2
ⴚ0.4
ⴚ0.04
ⴚ0.06
ⴚ0.08
ⴚ0.10
ⴚ0.12
ⴚ0.14
ⴚ0.16
ⴚ0.6
0
10
20
INPUT VOLTAGE – V
ⴚ0.18
0
30
TPC 9. 5 V Output Voltage Change vs. Input Voltage
REV. A
0.1
0.2
0.3
0.4
0.5
0.6
0.7
LOAD CURRENT – A
TPC 12. Load Regulation
–5–
0.8
0.9
1.0
ADP3050
0.8
SWITCH SATURATION VOLTAGE – V
VIN = 10V
0.7
VSW = 5V/DIV
0.6
0.5
0V
0.4
IL = 500mA/DIV
0.3
VIN = 10V
VOUT = 5V
ILOAD = 800mA
L = 33␮H
CIN = 22␮F
COUT = 100␮F
0.2
0A
0.1
0.0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
LOAD CURRENT – A
0.8
0.9
1.0
TIME – 1␮s/DIV
TPC 13. Switch Saturation Voltage vs. Load Current
TPC 16. Continuous Conduction-Mode Waveforms
210
VIN = 10V
ILOAD = 250␮A
SWITCHING FREQUENCY – kHz
208
VSW = 5V/DIV
206
204
0V
202
200
IL = 500mA/DIV
198
196
VIN = 10V
VOUT = 5V
ILOAD = 100mA
L = 33␮H
CIN = 22␮F
COUT = 100␮F
0A
194
192
190
ⴚ45 ⴚ35 ⴚ25 ⴚ15 ⴚ5 5 15 25 35 45 55
AMBIENT TEMPERATURE – ⴗC
65
75
85
TIME – 1␮s/DIV
TPC 14. Switching Frequency vs. Temperature
TPC 17. Discontinuous Conduction-Mode Waveforms
250
SWITCHING FREQUENCY – kHz
VIN = 10V
COMP = 0.4V
200
VOUT = 20mV/DIV
5V
150
ILOAD
100
1A
0A
50
0
0
0.2
0.4
0.6
0.8
NORMALIZED FEEDBACK VOLTAGE – V
VIN = 10V
VOUT = 5V
ILOAD = 100mA TO 1A SWITCHED
L = 33␮H
CIN = 22␮F
COUT = 100␮F
1.0
TIME – 400␮s/DIV
TPC 15. Frequency Foldback
TPC 18. Transient Response
–6–
REV. A
ADP3050
VIN = 10V
VOUT = 5V
VOUT = 1V/DIV
RLOAD = 19⍀
L = 33␮H COILTRONICS
UP2B-330
CIN = 22␮F
COUT = 100␮F
57.6
220
48.0
200
180
38.4
0V
IL = 500mA/DIV
0A
160
19.2
140
9.6
120
0
100
ⴚ9.6
80
ⴚ19.2
60
ⴚ28.8
40
ⴚ38.4
100
0
1k
10k
FREQUENCY – Hz
TIME – 100␮s/DIV
TPC 19. Start-Up from Shutdown
ADP3050 is drawn from the input supply. When the BIAS pin
is above 2.7 V, the majority of the operating current is then
drawn from this pin (usually tied to the regulator's low-voltage
output) instead of from the higher-voltage input supply. This
can provide substantial efficiency improvements at light-load
conditions, especially for systems where the input voltage is
much higher than the output voltage.
VIN = 10V, NO LOAD
1,450
TRANSCONDUCTANCE – ␮Mho
20
1M
100k
TPC 21. Error Amplifier Gain
1,500
1,400
1,350
1,300
The ADP3050 uses a special drive stage that allows the power
switch to saturate. An external diode and capacitor provide a
boosted voltage to the drive stage that is higher than the input
supply voltage. Overall efficiency is dramatically improved by
using this type of saturating drive stage.
1,250
1,200
1,150
1,100
1,050
1,000
ⴚ45 ⴚ35 ⴚ25 ⴚ15 ⴚ5
5
15 25 35 45
TEMPERATURE – ⴗC
55
65
75
85
Pulling the SD pin below 0.4 V puts the device in a low-power
mode, shutting off all internal circuitry and reducing the supply
current to under 20 µA.
TPC 20. Error Amplifier Transconductance vs. Temperature
3.3V
VOUT
L1
33␮H
THEORY OF OPERATION
The ADP3050 is a fixed-frequency, current-mode buck regulator.
Current mode systems provide excellent transient response, and
are much easier to compensate than voltage-mode systems. (Refer
to the functional block diagram.) At the beginning of each clock
cycle, the oscillator sets the latch, turning on the power switch.
The signal at the noninverting input of the comparator is a replica
of the switch current (summed with the oscillator ramp). When
this signal reaches the appropriate level set by the output of the
error amplifier, the comparator resets the latch and turns off the
power switch. In this manner, the error amplifier sets the correct
current trip level to keep the output in regulation. If the error
amplifier output increases, more current is delivered to the
output; if it decreases, less current is delivered to the output.
The current sense amplifier provides a signal proportional to
switch current to both the comparator and to a cycle-by-cycle
current limit. If the current limit is exceeded, the latch will be
reset, turning the switch off until the beginning of the next clock
cycle. The ADP3050 has a foldback current limit that reduces
the switching frequency under fault conditions to reduce stress
to the IC and to the external components.
D1
1N5818
+ C4
100␮F
D2
1N914
C3
220nF
1
SWITCH
2
BOOST
3
BIAS
4
FB
IN
8
GND
7
SD
6
COMP
5
U1
ADP3050-3.3
R1
4k⍀
C2
1nF
12V
VIN
+ C1
22␮F
Figure 1. Typical Application Circuit
Setting the Output Voltage
The output of the adjustable version (ADP3050AR) can be set
to any voltage between 1.25 V and 12 V by connecting a resistor
divider to the FB pin as shown in Figure 2.
V

R2 = R1 ×  OUT − 1
 1.2

Most of the control circuitry is biased from the 2.5 V internal
regulator. When the BIAS pin is left open, or when the voltage
at this pin is less than 2.7 V, all of the operating current for the
REV. A
PHASE – Degrees
MAGNITUDE – dB
NO LOAD
28.8
–7–
(1)
ADP3050
L1
22␮H
D1
1N5817
C3
0.22␮F
R2
21.5k⍀
CF
D2
1N4148
Where VIN(MAX) is the maximum input voltage, VOUT is the regulated output voltage, and fSW is the switching frequency (200 kHz).
The initial choice for the amount of ripple current may seem arbitrary, but it will serve as a good starting point for finding a standard
off-the-shelf inductor value (i.e., 10 µH, 15 µH, 22 µH, 33 µH, and
47 µH). If a specific inductance value is to be used, simply rearrange
the above equation to find the ripple current. For an 800 mA, 12 V
to 5 V system, and a ripple current of 320 mA (40% of 800 mA) is
chosen, the inductance would be:
2.5V
VOUT
C4
+
2 ⴛ 22␮F
CERAMIC
1
SWITCH
2
BOOST
3
BIAS
4
FB
R1
20k⍀
IN
8
GND
7
SD
6
COMP
5
U1
ADP3050
RC
7.5k⍀
12 − 5
1
5
×
×
= 45.5 µH
3
0.32 200 × 10
12
A 47 µH inductor is the closest standard value, which gives a ripple
current of about 310 mA. The peak switch current is equal to the
load current plus one-half the ripple current (this is also the peak
current for the inductor and the catch diode):
L=
CC
4.7nF
5V
VIN
+ C1
2 ⴛ 10␮F
CERAMIC
C2
0.01␮F
GND
1
IRIPPLE
2
(3)
= 0.8 + 0.155 = 0.95 A
Pick an inductor with a dc (or saturation) current rating about
20% larger than ISW(PK) to ensure that the inductor is not running
near the edge of saturation. For this example, 1.20 ⫻ 0.95 A =
1.14 A, so use an inductor with a dc current rating of at least 1.2 A.
The maximum switch current is internally limited to 1.5 A, and
this limit, along with the ripple current, will determine the maximum load current the system can provide.
I SW(PK) = IOUT(MAX) +
Figure 2. Adjustable Output Application Circuit
APPLICATION INFORMATION
The complete process for designing a step-down switching regulator using the ADP3050 is given in the following sections. Each
section includes a list of recommended devices. These lists do
not include every available device, nor every available manufacturer. They contain only surface-mount devices, but equivalent
through-hole devices can be substituted if needed. In choosing
components, keep in mind what is most important to the design
(efficiency, cost, size, etc.) as these things will ultimately determine which components are used. Also, make sure the design
specifications are clearly defined and that they reflect the worstcase conditions. Key specifications include the minimum and
maximum input voltage, the output voltage and ripple, and the
minimum and maximum load current.
If the load current decreases to below one-half the ripple current,
the regulator will operate in discontinuous mode.
Discontinuous Mode
For load currents less than around 0.5 A, discontinuous mode
operation can be used. This will allow the use of a smaller inductor, but the ripple current will be much higher (which means a
higher output ripple voltage). If a larger output capacitor must be
used to reduce the output ripple voltage, the overall system may
actually take up more board area than if a larger inductor was
used. The operation and equations for the two modes are quite
different, but the boundary between these two modes occurs
when the ripple current is equal to twice the load current (when
IRIPPLE = 2 ⫻ IOUT). From this we can use Equation 2 to find the
minimum inductor value needed to keep the system in continuous mode operation (solve for the inductor value with IRIPPLE =
2 ⫻ IOUT).
INDUCTOR SELECTION
The inductor value will determine the mode of operation for the
regulator: continuous mode, where the inductor current flows
continuously; or discontinuous mode, where the inductor current
reduces to zero during every switch cycle. Continuous mode is
the best choice for many applications. It provides higher output
power, lower peak currents in the switch, inductor, and diode,
and a lower inductor ripple current (which means lower output
ripple voltage). Discontinuous mode does allow the use of smaller
magnetics, but at a price: lower available load current, and higher
peak and ripple currents. Designs with a high input voltage or a
low load current often operate in discontinuous mode to minimize inductor value and size. The ADP3050 is designed to work
well in both modes of operation.
LDIS =
VIN (MAX) − VOUT
2 × IOUT
LDIS ≤
The inductor current in a continuous mode system is a triangular
waveform (equal to the ripple current) centered around a dc value
(equal to the load current). The amount of ripple current is determined by the inductor value, and is usually between 20% and 40%
of the maximum load current. To reduce the inductor size, ripple
currents between 40% and 80% are often used in continuous
mode designs with a high input voltage or a low output current.
The inductor value can be calculated using the following equation:
L=
IRIPPLE
×
1
f SW
×
VOUT
VIN (MAX)
VOUT
1
×
f SW VIN (MAX)
(4)
Using an inductor below this value will cause the system to operate
in discontinuous mode. For a 400 mA, 24 V to 5 V system:
Continuous Mode
VIN (MAX) − VOUT
×
24 − 5
1
5
×
×
2 × 0.4 200 × 10 3 24
≤ 24.7 µH
If the chosen inductor value is too small, the internal current
limit will trip each cycle and the regulator will have trouble
providing the necessary load current.
Inductor Core Types and Materials
Many types of inductors are currently available. Numerous core
styles along with numerous core materials often make the selection process seem even more confusing. A quick overview of the
(2)
–8–
REV. A
ADP3050
types of inductors available will make the selection process a
little easier to understand.
Open-core geometries (bobbin core) are usually less expensive than
closed-core geometries (toroidal core) and can be a good choice for
some applications, but care must be taken when they are used. In
open-core inductors, the magnetic flux is not completely contained
inside the core. The radiating magnetic field will generate ElectroMagnetic Interference (EMI), often inducing voltages onto nearby
circuit board traces. These inductors may not be suitable for systems
that contain very high accuracy circuits or sensitive magnetics. A few
manufacturers have “semiclosed” and “shielded” cores, where an
outer magnetic shield surrounds a bobbin core. These devices have
less EMI than the standard open core, and will usually be smaller
than a closed core.
Most core materials used in surface-mount inductors are either
powdered iron or ferrite. For many designs, material choice will
be arbitrary, but the properties of each material should be recognized. Ferrites will have lower core losses than powdered iron,
but the lower loss means a higher price. Powdered iron cores will
saturate softly (the inductance gradually reduces as current rating
is exceeded), while ferrite cores will saturate much more abruptly
(the inductance rapidly reduces). Kool Mµ® is one type of ferrite
that is specially designed to minimize core losses and heat generation (especially at switching frequencies above 100 kHz), but again,
these devices will be more expensive.
Do not overlook the dc winding resistance (DCR) of the inductor.
A high DCR can decrease the system efficiency by 2%–5% for
lower output voltages at heavy loads. To obtain a lower DCR
means using a physically larger inductor, so a trade-off in size
and efficiency must be made. The power loss due to this resistance is simply IOUT2 ⫻ DCR. For an 800 mA, 5 V to 3.3 V
system with an inductor DCR of 100 mΩ, the winding resistance will dissipate (0.82 ⫻ 0.1 Ω) = 64 mW. This represents a
power loss to the system of 64 mW/(3.3 V ⫻ 800 mA) = 2.4%.
Typical DCR values will be between 10 mΩ and 200 mΩ.
Choosing an Inductor
Several considerations must be made when choosing an inductor:
cost, size, EMI, core and copper losses, and maximum current
rating. Follow the steps below to choose an inductor that is right
for the system (refer to the calculations and descriptions from the
previous sections). Table I shows an extensive list of inductors
that can be used. Contact the manufacturers for their full product
offering, availability and pricing. They offer many more values
and package sizes to suit numerous applications.
1. Choose a mode of operation, then calculate the inductor
value using the appropriate equation. For continuous mode
systems, a ripple current of 40% the maximum load current
is a good starting point. The inductor value can then be
increased or decreased if desired.
2. Calculate the peak switch current (this will be the maximum
current seen by the inductor). Make sure that the dc (or
saturation) current rating of the inductor is high enough
(around 1.2 times the peak switch current). Inductors with
dc current ratings of at least 1 A should be used for all designs.
This will provide a safety margin for start-up and fault conditions where the inductor current will be higher than normal.
If an inductor’s current rating is exceeded, the core will
saturate, causing the inductance value to decrease and the
inductor’s temperature to increase.
3. Estimate the dc winding resistance based on the inductance
value. A good rule of thumb is to allow about 5 mΩ of resistance per µH of inductance.
4. Pick the core material and type. First decide if an open-core
inductor can be used with the design. If you are not sure,
you can always get a few samples of each type (open core,
semi-closed core, shielded core, and closed core) and try
them out. Do not be discouraged from using open core
inductors simply because they require a little extra care; just
be aware of what to look for if you do use them. They are
quite small and inexpensive, and are used successfully in
many different applications.
OUTPUT CAPACITOR SELECTION
The ADP3050 can be used with any type of output capacitor.
The trade-offs between price, component size, and regulator
performance can be evaluated to determine the best choice for
each application. The Effective Series Resistance (ESR) of the
capacitor plays an important role in both the loop compensation
and the system performance. The ESR provides a “zero” in the
feedback loop, therefore the ESR value must be known so that
the loop can be compensated correctly (most manufacturers
specify maximum ESR in their data sheets). The capacitor ESR
also contributes to the output ripple voltage (VRIPPLE = ESR ⫻
IRIPPLE). Solid tantalum or multilayer ceramic capacitors are
recommended, providing good performance with a small size
and reasonable cost.
Solid tantalum capacitors have a good combination of low ESR
and high capacitance, and are available from several different manufacturers (AVX TPS series, Sprague 593D series, Kemet T495
series, NEMCO LSR series). Capacitance values from 22 µF to more
than 500 µF can be used, but values of 47 µF to 220 µF will be
sufficient for most designs. A smaller value can be used, but ESR is
size-dependent, so a smaller device will have a higher ESR. Ensure
that the capacitor’s ripple current rating is larger than the inductor
ripple current (the ripple current will flow into the output capacitor).
Multilayer ceramic capacitors can be used in applications where
minimum output voltage ripple is a priority. They have a very low
ESR (a 22 µF ceramic can have an ESR one-fifth that of a 22 µF
solid tantalum), but may require more board area for the same
value of output capacitance. A few manufacturers have recently
improved upon their low voltage ceramic capacitors, providing a
smaller package with a lower ESR (Tokin, Murata, Taiyo Yuden
and AVX). Several ceramics can be used in parallel to give an
extremely low ESR and a good value of capacitance. If your design
is very cost-sensitive and not severely space-limited, several aluminum electrolytic capacitors can be used in parallel (their size and
ESR are larger than ceramic and solid tantalum). OS-CON
capacitors can also be used, but they are typically larger and
more expensive than ceramic or solid tantalum capacitors.
Choosing an Output Capacitor
Use the following steps to choose an appropriate capacitor.
Several choices for output capacitors are contained in Table III.
1. Decide the maximum output ripple voltage for the design,
and this will determine your maximum ESR (remember
that VRIPPLE ≈ ESR ⫻ IRIPPLE). Typical output ripple voltages
range between 0.5% and 2% of the output voltage. To lower
the output voltage ripple, there are only two choices: either
increase the inductor value, or use an output capacitor with a
lower ESR.
Kool Mµ is a registered trademark of Magnetics, Inc.
REV. A
–9–
ADP3050
Table I. Inductor Selection Guide
Vendor/
Model
Value
(␮H)
Max
IDC
(A)
Max
DCR
(⍀)
Core
Type
Core
Material
Package
Dimensions (mm)
W
L
H
Sumida
CD73
CD73
CD73
CR75
CR75
CR75
CDRH73
CDRH73
CDRH6D38
CDRH6D38
CDR105B
CDR105B
CDR105B
10
15
22
22
33
47
10
15
22
33
22
33
47
1.4
1.2
1.1
1.5
1.2
1.1
1.7
1.3
1.3
1.1
1.4
1.2
1.0
0.08
0.10
0.13
0.11
0.13
0.18
0.08
0.13
0.10
0.12
0.08
0.11
0.14
Open
Open
Open
Open
Open
Open
S.C.
S.C.
S.C.
S.C.
S.C.
S.C.
S.C.
Ferrite
Ferrite
Ferrite
Ferrite
Ferrite
Ferrite
Ferrite
Ferrite
Ferrite
Ferrite
Ferrite
Ferrite
Ferrite
7.0
7.0
7.0
7.0
7.0
7.0
7.3
7.3
6.7
6.7
9.0
9.0
9.0
7.8
7.8
7.8
7.8
7.8
7.8
7.3
7.3
6.7
6.7
10.0
10.0
10.0
3.5
3.5
3.5
5.0
5.0
5.0
3.4
3.4
4.0
4.0
5.0
5.0
5.0
COILCRAFT
DO1608
DO3316
DO3316
DO3316
DO3316
DO3316
DT3316
DT3316
10
10
15
22
33
47
10
15
1.1
3.8
3.0
2.6
2.0
1.6
2.0
1.8
0.14
0.03
0.04
0.05
0.09
0.14
0.06
0.06
Open
Open
Open
Open
Open
Open
S.C.
S.C.
Ferrite
Ferrite
Ferrite
Ferrite
Ferrite
Ferrite
Ferrite
Ferrite
4.6
9.4
9.4
9.4
9.4
9.4
9.4
9.4
6.6
13.0
13.0
13.0
13.0
13.0
13.0
13.0
2.9
5.1
5.1
5.1
5.1
5.1
5.1
5.1
COILTRONICS*
CTX10-1
CTX20-1
CTX10-2
CTX20-2
CTX33-2
CTX10-2
CTX10-1P
CTX15-1P
CTX20-1P
CTX20-2P
UP2-330
UP2-470
10
20
10
20
33
40
10
15
20
20
33
47
1.9
1.0
2.5
1.3
1.5
1.3
1.6
1.2
1.0
1.3
1.7
1.4
0.04
0.14
0.03
0.11
0.09
0.12
0.03
0.05
0.08
0.11
0.10
0.15
Toroid
Toroid
Toroid
Toroid
Toroid
Toroid
Toroid
Toroid
Toroid
Toroid
Open
Open
Kool Mµ
Kool Mµ
Kool Mµ
Kool Mµ
Kool Mµ
Kool Mµ
P.I.
P.I.
P.I.
P.I.
Ferrite
Ferrite
8.9
8.9
8.9
8.9
8.9
8.9
8.9
8.9
8.9
8.9
8.8
8.8
8.9
8.9
8.9
8.9
8.9
8.9
8.9
8.9
8.9
8.9
10.6
10.6
4.2
4.2
6.0
6.0
6.0
6.0
4.2
4.2
4.2
6.0
5.9
5.9
TOKIN
SSB64
SSB64
SSB84
SSB84
SSB84
10
15
10
15
22
1.2
1.0
1.4
1.2
1.2
0.12
0.15
0.10
0.11
0.16
Open
Open
Open
Open
Open
Ferrite
Ferrite
Ferrite
Ferrite
Ferrite
6.3
6.3
8.3
8.3
8.3
6.3
6.3
8.3
8.3
8.3
6.0
6.0
6.0
6.0
6.0
S.C. = semiclosed, P.I. = powdered iron, Toroid is a closed core.
*Coiltronics toroidal inductors consist of two windings on one core that can be connected in parallel (for a higher current rating) or in series (for a higher inductance value);
consult Coiltronics data sheet.
Table II. Inductor Manufacturers
Company
Phone
Fax
Web Site
Sumida (USA)
Sumida (Japan)
Coilcraft
Coiltronics
Tokin (USA)
Tokin (Japan)
(847) 956-0666
81-3-3607-5111
(847) 639-6400
(561) 241-7876
(408) 432-8020
81-22-211-1281
(847) 956-0702
81-3-3607-5144
(847) 639-1469
(561) 241-9339
(408) 434-0375
81-22-211-0975
www.sumida.com
www.sumida.com
www.coilcraft.com
www.coiltronics.com
www.tokin.com
www.tokin.com
–10–
REV. A
ADP3050
voltage and 1 A average forward current. For lower input voltages,
use a lower voltage Schottky to reduce the diode forward voltage
drop and increase overall system efficiency (i.e., a 12 V to 5 V
system does not need a 30 V diode). For automotive applications,
a 60 V Schottky may be necessary. The average forward current for
the catch diode can be calculated by:
2. Decide what type of capacitor to use (tantalum, ceramic,
etc.), then look at the table for some possible devices. Many
more values, sizes, and voltage ratings are available, so contact
each manufacturer for a complete product list. If a certain type
of capacitor must be used and space permits, simply use
several devices in parallel to reduce the total ESR.
3. Check the capacitor voltage rating and ripple current rating
to ensure it will work for your application (these ratings are
derated for higher temperatures, so always check the
manufacturer’s data sheet).
IDIODE(AVG) = IOUT ×
VIN – VOUT
VIN
(5)
For the earlier continuous mode example (12 V to 5 V at 800 mA),
the average diode current would be:
4. Make sure the final choice for the output capacitor has been
optimized for cost, size, availability, and performance while
still meeting the required capacitance. The recommended
capacitance is in the 47 µF to 220 µF range.
IDIODE(AVG) = 0.8 ×
12 – 5
= 0.47 A
12
For this system, a 1N5817 would be a good choice (rated at 20 V
and 1 A). Do not use catch diodes rated less than 1 A. Even though
the average current can be less than 1 A under normal operating
conditions, since the diode current will be much higher under fault
conditions. The worst case fault condition for the diode occurs when
the regulator becomes slightly overloaded (sometimes called a soft
CATCH DIODE SELECTION
The recommended catch diode is a type 1N5818 Schottky or an
equivalent. The low forward voltage drop (450 mV typical at 1 A)
and fast switching speed of a Schottky rectifier provide the best
performance and efficiency. The 1N5818 is rated at 30 V reverse
Table III. Capacitor Selection Guide
Vendor/
Series
Value
(␮F)
ESR*
(⍀)
Max
Voltage
(V)
Type
Package
Dimensions (mm)
W
L
H
AVX
TPS
TPS
TPS
TPS
Y5V
Y5V
Y5V
Y5V
100
47
100
100
10
10
18
22
0.150
0.150
0.100
0.125
~0.040
~0.040
~0.040
~0.040
6.3
16
10
16
10
16
10
10
Tantalum
Tantalum
Tantalum
Tantalum
MLC
MLC
MLC
MLC
3.2
4.3
4.3
4.3
1.6
2.5
2.5
2.5
6.0
7.3
7.3
7.3
3.2
3.2
3.2
3.2
2.6
2.9
2.9
2.9
1.5
1.7
1.7
1.7
Sprague
593D
593D
593D
593D
47
68
100
100
0.150
0.150
0.100
0.100
16
16
10
16
Tantalum
Tantalum
Tantalum
Tantalum
4.3
4.3
4.3
4.3
7.3
7.3
7.3
7.3
2.8
2.8
2.8
4.0
Tokin
CU
CU
CU
CU
CU
10
10
18
10
22
~0.040
~0.040
~0.040
~0.040
~0.030
10
25
25
50
25
MLC
MLC
MLC
MLC
MLC
1.6
2.7
5.0
5.0
5.0
3.2
5.7
5.7
5.7
5.7
1.6
2.5
2.5
3.0
3.0
*Maximum ESR ratings at 100 kHz; MLC = multilayer ceramic.
Table IV. Capacitor Manufacturers
Company
Phone
Fax
Web Address
AVX
Kemet
Murata (USA)
Nemco
Sprague
Tokin (USA)
Tokin (Japan)
Taiyo Yuden (USA)
Taiyo Yuden (Japan)
(803) 448-9411
(864) 963-6300
(800) 831-9172
(800) 227-4058
(207) 324-4140
(408) 432-8020
81-22-211-1281
(800) 348-2496
81-33-833-5441
(803) 448-1943
(864) 963-6521
(770) 436-3030
(650) 571-0825
(207) 324-7223
(408) 434-0375
81-22-211-0975
(847) 925-0899
81-33-835-4754
www.avxcorp.com
www.kemet.com
www.murata.com
www.nemcocaps.com
www.vishay.com
www.tokin.com
www.tokin.com
www.t-yuden.com
www.t-yuden.com
REV. A
–11–
ADP3050
short). This is usually only a problem when the input voltage to output voltage ratio is greater than 2.5. Under this condition, the load
current needed is slightly more than the regulator can provide. The
output voltage then droops slightly, and the switch stays on every
cycle until the internal current limit is reached. Under this condition,
the load current can reach around 1.2 A. For example: a system with
an input voltage of 24 V and an output voltage of 5 V, if a gradual
overload causes the output voltage to droop to 4 V, the average
diode current would be:
IDIODE(AVG) = 1.2 ×
24 – 4
= 1.0 A
24
If the system must survive such gradual overloads for a prolonged
period of time, ensure that the diode chosen can survive these
conditions. A larger 2 A or 3 A diode can be used if necessary.
Choosing a Catch Diode
Use the following steps to pick an appropriate catch diode.
Table V shows several Schottky rectifiers with different reverse
voltage and forward current ratings.
1. The average diode current rating must be sufficient to provide
the required load current (see above calculations). Diodes
rated below 1 A should not be used, even if the average diode
current is much lower.
2. The reverse voltage rating of the catch diode should be at
least the maximum input voltage. Often a higher rating is
chosen (1.2 times the maximum input voltage) to provide a
safety margin.
When operating in discontinuous mode, high frequency ringing
will appear at the switch node when the inductor current has
decreased to zero. This ringing is normal, and is not a result of
loop instability. It is caused by the switch and diode capacitance
reacting with the inductor to form a damped sinusoidal ringing.
This ringing is usually in the range of several megahertz, and is
not harmful to normal circuit operation.
The input bypass capacitor plays an important role in proper
regulator operation, minimizing voltage transients at the input
and providing a short local loop for the switching current. Place
this capacitor close to ADP3050 between the VIN and GND pins
using short, wide traces. This input capacitor should have an rms
ripple current rating of at least:
VOUT VOUT 
−

VIN
 VIN 
Ceramics are an excellent choice for input bypassing due to their
low ESR and high ripple current rating. Ceramics are especially
suited for high input voltages, and are available from many different manufacturers. Tantalums are often used for input bypassing,
but precautions must be taken, as they occasionally fail when
subjected to large inrush currents during power-up. These
surges are common when the regulator input is connected to a
battery or high-capacitance supply. Several manufacturers now
offer surface-mount solid tantalum capacitors that are surge
tested (AVS TPS series, Sprague 593D series, Kemet T495 series,
and NEMCO LSR series), but even these devices can fail if the
current surge occurs when the capacitor voltage is near its maximum rating. For this reason, a 2:1 derating is suggested for
tantalum capacitors used in applications where large inrush currents
are present (i.e., a 20 V tantalum should only be used for an input
voltage up to 10 V). Aluminum electrolytics are the cheapest choice,
but it takes several in parallel to get a good rms current rating.
OS-CON capacitors have a good ESR and ripple current rating,
but they are typically larger and more costly. Refer to Table IV
for a list of capacitor manufacturers.
DISCONTINUOUS MODE RINGING
INPUT CAPACITOR SELECTION
ICIN(RMS) ≥ IOUT ×
This rating is crucial, as the input capacitor must be able to
withstand the large current pulses present at the input of a stepdown regulator. Values of 20 µF to 50 µF are typical, but the
main criteria for capacitor selection should be the ripple current
and voltage ratings.
SETTING THE OUTPUT VOLTAGE
2
(6)
The fixed voltage versions of the ADP3050 (3.3 V and 5 V) have
the feedback resistor divider included on-chip. For the adjustable
version, the output voltage is set using two external resistors.
Referring to Figure 2, pick a value for R1 between 10 kΩ and
20 kΩ, then calculate the appropriate value for R2 using:
V

R2 = R1 ×  OUT − 1
 1.20

Table V. Schottky Diode Selection Guide
VR
1 A Diodes
2 A Diodes
15 V
10BQ15
30BQ15
20 V
1N5817
SK12
B120
EC10QS02
B220
V1N5818
SK13
B130
MBRS130
EC10QS03
B230
EC21QS03
NSQ03A03
1N5819
SK14
B140
MBRS140
10BQ040
EC10QS04
B240
EC21QS04
30 V
40 V
3 A Diodes
It is important to note that the accuracy of these resistors directly
affects the accuracy of the output voltage. The FB pin threshold
variation is ± 3%, and the tolerances of R1 and R2 will add to this
SK32
B320
NSQ03A02
SK33
B330
SK34
B340
MBRS340
30BQ040
NSQ03A04
(7)
Table VI. Schottky Diode Manufacturers
Company
Phone
Fax
Motorola
MBRSxxx
(602) 244-3576
(602) 244-4015 www.mot.com
Diodes, Inc.
1N58xx, Bxxx, SKxxx
(805) 446-4800
(805) 446-4850 www.diodes.com
International Rectifier
10BQxxx, 30BQxxx
(310) 322-3331
(310) 322-3332 www.irf.com
Nihon Inter Electronic (USA)
Nihon Inter Electronic (Japan)
ECxxxxxx, NSQxxxx
(661) 867-2555 (661) 867-2698
81-33-343-3411 81-33-343-7377
–12–
REV. A
ADP3050
to determine the total output variation. Use 1% resistors placed
close to the FB pin to prevent noise pickup.
If this ripple voltage were more than 100 mV, RC would need to
be decreased to prevent subharmonic switching. Typical values
for RC will be in the range of 2 kΩ to 10 kΩ.
FREQUENCY COMPENSATION
For output voltages greater than 5 V, it may be necessary to add a
small capacitor in parallel with R2, as shown in Figure 2. This
will improve stability and transient response. For tantalum output
capacitors, the typical value for CF is 100 pF. For ceramic output
capacitors, the typical value for CF is 400 pF.
The ADP3050 uses a unique compensation scheme that allows the
use of any type of output capacitor. The designer is not limited to a
specific type of capacitor nor a specific ESR range. External compensation allows the designer to optimize the loop for transient response
and system performance. The values for RC and CC will set the
pole and zero locations for the error amplifier to compensate the
regulator loop.
For tantalum output capacitors, the typical compensation values
are RC = 4 kΩ and CC = 1 nF; for ceramics, the typical values
are RC = 4 kΩ and CC = 4.7 nF. These values may not be optimized for all designs, but they should provide a good starting
point for selecting the final compensation values. Other types of
output capacitors will require different values of CC between
0.5 nF and 10 nF. Typically, the lower the ESR of the output
capacitor, the larger the value for CC. Normal variations in
capacitor ESR, output capacitance, and inductor value (due
to production tolerances, changes in operating point, changes
in temperature) will affect the loop gain and phase response.
Always check the final design over its complete operating range
to ensure proper regulator operation.
Adjusting the RC and CC values can optimize the compensation for
your system. Use the typical values above as a starting point, then
try increasing and decreasing each independently and observing the
transient response. An easy way to check the transient response of
the design is by observing the output while pulsing the load current
at a rate of around 100 Hz to 1 kHz. There should be some slight
ringing at the output when the load pulses, but this should not be
excessive (just a few rings). The frequency of this ringing shows
the approximate unity gain frequency of the loop. Again, always
check the design over its full operating range of input voltage,
output current, and temperature to ensure that the loop is compensated correctly.
In addition to setting the zero location, RC also sets the high
frequency gain of the error amplifier. If this gain is too large,
output ripple voltage will appear at the COMP pin (the output
of the error amplifier) with enough amplitude to interfere with normal regulator operation. If this happens, subharmonic switching
will occur (the pulsewidth of the switch waveform will change, even
though the output voltage stays regulated). The voltage ripple at
the COMP pin should be kept below about 100 mV to prevent
this from occurring. The amount of ripple can be estimated by
the following formula, where gm is the error amplifier transconductance (gm = 1,250 µMho):
VCOMP, RIPPLE = ( g m × RC ) × ( IRIPPLE × ESR ) ×
VFB
(8)
VOUT
For example: a 12 V to 5 V, 800 mA regulator with an inductor
of L = 47 µH has IRIPPLE = 310 mA (example from earlier section);
if a 100 µF tantalum output capacitor with a maximum ESR of
100 mΩ and compensation values of RC = 4 kΩ and CC = 1 nF
are used. The ripple voltage at the COMP pin will be:
(
)
VCOMP, RIPPLE = 1, 250 × 10 −6 × 4 × 10 3 × (0.310 × 0.1)
1.20
×
= 37.2 mV
5.0
REV. A
CURRENT LIMIT/FREQUENCY FOLDBACK
The ADP3050 uses a cycle-by-cycle current limit to protect the
device under fault and high stress conditions. When the current
limit is exceeded, the power switch turns off until the beginning
of the next oscillator cycle. If the voltage on the feedback pin
drops below 80% of its nominal value, the oscillator frequency
starts to decrease (see TPC 15 in the Typical Performance
Characteristics section). The frequency gradually reduces to a
minimum value of around 80 kHz (this minimum occurs when
the feedback voltage falls to 30% of its nominal value). This
reduces the power dissipation in the IC, the external diode, and
the inductor during short circuit conditions. This frequency
foldback method provides complete device fault protection without interfering with the normal device operation.
BIAS PIN CONNECTION
To help improve efficiency, most of the internal operating current
can be drawn from the lower voltage regulated output voltage
instead of from the input supply. For example, if the input voltage
is 24 V and the output voltage is 5 V, a quiescent current of 4 mA
will waste 96 mW if drawn from the input supply, but only 20 mW
is drawn from the regulated 5 V output. This power savings will be
most evident at high input voltages and low load currents. The output voltage must be 3 V or higher to take advantage of this feature.
BOOSTED DRIVE STAGE
An external capacitor and diode are used to provide the boosted
voltage needed for the special drive stage. If the output voltage is
above 4 V, connect the anode of the boost diode to the regulated
output; for output voltages less than or equal to 3 V, connect it to
the input supply. For some low voltage systems (i.e., 5 V to 3.3 V
converters), the anode of the boost diode can be connected to
either the input or output voltage. During switch off-time, the
boost capacitor is charged up to the voltage at the anode of the
boost diode. When the switch turns on, this voltage is added to
the switch voltage (the boost diode is reverse-biased) providing a
voltage higher than the input supply. The peak voltage appearing
on the BOOST pin will be the sum of the input voltage and the
boost voltage (either VIN + VOUT or 2 ⫻ VIN). Ensure that this peak
voltage does not exceed the BOOST pin maximum rating of 45 V.
For most applications, a 1N4148 or 1N914 type diode can be
used with a 220 nF capacitor. A 470 nF capacitor may be needed
for output voltages between 3 V and 4 V. The boost capacitor
should have an ESR less than 2 Ω to ensure that it will be adequately
charged up during switch off-time. Most any type of film or ceramic
capacitor can be used.
START-UP/MINIMUM INPUT VOLTAGE
For most designs, the regulated output voltage provides the
boosted voltage for the drive stage. During startup, the output
voltage is zero, so there is no boosted supply for the drive stage.
–13–
ADP3050
To deal with this problem, the ADP3050 contains a backup
drive stage to get everything started. As the output voltage
increases, so will the boost voltage. When the boost voltage
reaches around 2.5 V, the switch drive will transition smoothly
from the backup driver to the boosted driver. If the boost voltage
should decrease below around 2.5 V (i.e., short circuit, overload
condition), the backup stage will again take over to provide
switch drive. The minimum input voltage needed for the ADP3050
to function correctly is about 3.6 V (this will ensure proper operation of the internal circuitry), but a small amount of headroom
is needed for all step-down regulators. The following formula
gives the approximate minimum input voltage needed for a
given system, where VSAT is the switch saturation voltage (see
TPC 13 for the appropriate value of VSAT). TPC 11 also shows the
typical minimum input voltage needed for 3.3 V and 5 V systems.
VIN (MIN) =
VOUT + VSAT
0.85
(9)
THERMAL CONSIDERATIONS
Several factors contribute to IC power dissipation: ac and dc
switch losses, boost current, and quiescent current. The following
formulas can be used to calculate these losses to determine the
power dissipation of the IC. These formulas assume continuous
mode operation, but they provide a reasonable estimate for discontinuous mode systems (do not use these formulas to calculate
efficiency at light loads).
Switch loss:


V
PSW =  IOUT × VSAT × OUT  + (tOV × IOUT × VIN × f SW ) (10)
VIN 

Boost current loss:
PBOOST =
IOUT VOUT
×
β SW
VIN
2
(11)
The ADP3050 uses a thermally enhanced SO-8 package with a
package thermal resistance, θJA, of around 80°C/W for a fourlayer board (poor layout techniques will result in a higher thermal
resistance). This allows the ADP3050 to provide 1 A load currents
in an SO-8 package. The maximum die temperature, TJ, can be
calculated using the thermal resistance and the maximum ambient
temperature:
TJ = TA + θ JA × PTOTAL
For the previous example (5 V to 3.3 V at 800 mA system, SO-8
thermally enhanced package using good layout techniques) with
a worst-case ambient temperature of 70°C:
TJ = 70°C + 80°C/W × 0.41 = 103°C
The maximum operating junction (die) temperature is 125°C, so
this system will operate within the safe limits of the ADP3050.
Check the die temperature at minimum and maximum supply
voltages to ensure proper operation under all conditions. The PC
board and its copper traces will provide sufficient heat-sinking,
but be sure to follow the layout suggestions in the Board Layout
Guidelines section. For any design that combines high output
current with high duty cycle and/or high input voltage, the junction temperature must be calculated to ensure normal operation.
Always use the equations in this section to estimate the power
dissipation.
BOARD LAYOUT GUIDELINES
A good board layout is essential when designing a switching
regulator. The high switching currents along with parasitic
wiring inductances can generate significant voltage transients and
cause havoc in sensitive circuits. For best results, keep the main
switching path as tight as possible (keep L1, D1, CIN, and COUT
close together) and minimize the copper area of the SWITCH and
BOOST nodes (without violating current density requirements) to
reduce the amount of noise coupling into other sensitive nodes.
Quiescent current loss:
L1
(
)
PQ = VIN × IQ + (VOUT × I BIAS )
VIN
(12)
where VSAT is ~0.6 V at IOUT = 800 mA (taken from TPC 13), fSW is
the switch frequency (200 kHz), tOV is the switch current/voltage
overlap time (~50 ns), β SW is the current gain of the NPN power
switch (~50), IQ is the quiescent current drawn from VIN (~1 mA)
and IBIAS is the quiescent current drawn from VOUT (~4 mA).

3.3 
PSW =  0.8 × 0.6 ×
+

5.0 
−9
PBOOST =
(
)
0.8 3.32
×
= 35 mW
50
5.0
)
PQ = 5 × 10 −3 + 3.3 × 4 × 10 −3 = 18 mW
For a total IC power dissipation of:
PTOTAL = PSW + PBOOST + PQ
= 410 mW
VOUT
SWITCH
ADP3050
D1
COUT
GND
GND
GND
Figure 3. Main Switching Path
× 0.8 × 5.0 × 200 × 10 3 = 357 mW
) (
IN
CIN
For example: for a 5 V to 3.3 V system with IOUT = 800 mA:
(50 × 10
(14)
(13)
The external components should be located as close to the
ADP3050 as possible. For best thermal performance, use wide
copper traces for all IC connections, and always connect the
GND pin to a large piece of copper or ground plane. The additional copper will improve heat transfer from the IC, greatly
reducing the package thermal resistance. Further improvements
of the thermal performance can be made by using multilayer
boards and using vias to transfer heat to the other layers. A
single layer board layout is shown in Figure 4. The amount of
copper used for the input, output, and ground traces can be
reduced, but were made large to improve the thermal performance. For the 5 V and 3.3 V versions, leave out R1 and R2;
for the Adjustable version, remove the trace that shorts out R2.
Route all sensitive traces and components, such as those associated
with the feedback and compensation away from the BOOST and
SWITCH traces.
–14–
REV. A
ADP3050
GROUND
OUTPUT
its operation is quite different. For this topology, the feedback
pin is grounded and the GND pin is tied to the negative output,
allowing the feedback network of the IC to regulate the negative
output voltage.
INPUT
C1
L1
47␮H
D2
1N4148
C5
100␮F
C3
0.22␮F
C3
L1
D1
1N5818
NC
1
SWITCH
2
BOOST
3
BIAS
4
FB
IN
8
GND
7
SD
6
COMP
5
U1
ADP3050-5
D1
R1
5.1k⍀
+
C4
3.3nF
VOUT
D2
C2
ⴚ5V @ 0.5A
SD
12V
VIN
+ C1
C2
0.01␮F
22␮F
R2
R1
CC
GND
RC
ADP3050
Figure 6. Inverting (Buck-Boost) Regulator
Figure 4. Recommended Board Layout
TYPICAL APPLICATIONS
5 V to 3.3 V Buck (Step-Down) Regulator
The circuit in Figure 5 shows the ADP3050 in a buck configuration. It is used to generate 3.3 V regulated output from 5 V
input voltage with the following specifications:
VIN = 4.5 V to 5.5 V
VOUT = 3.3 V
IOUT = 0.75 A
IRIPPLE = 0.4 A ⫻ 0.75 A = 0.3 A
VOUT RIPPLE = 50 mV
L1
22␮H
D1
1N5817
3.3V
VOUT
+ C5
100␮F
D2
1N4148
C3
0.22␮F
1
SWITCH
2
BOOST
3
BIAS
4
FB
IN
8
GND
7
SD
6
COMP
5
U1
ADP3050-3.3


VIN × VOUT
(15)
 I SW (MAX) −


2 × f SW × L × VIN + VOUT 


where ISW(MAX) is the switch current limit rating of the ADP3050
and VIN is the minimum input voltage. The inductor ripple current
can be estimated using the following equation:
(
R1
7.5k⍀
5V
C2
0.01␮F
GND
Figure 5. 5 V to 3.3 V Buck Regulator
INVERTING (BUCK-BOOST) REGULATOR
VIN
×
VIN + VOUT
VIN (MAX)
L
×
)
VOUT
1
×
f SW VIN (MAX) + VOUT
(16)
For the circuit in Figure 6, the maximum ripple current (at the
maximum input voltage) is:
VIN
22␮F
IOUT (MAX) =
IRIPPLE =
SD
+ C1
The design procedure used for the standard buck converter cannot
be used for a buck-boost converter due to fundamental differences
in how the output voltage is generated. The switch currents in the
buck-boost are much higher than in the standard buck converter,
thus lowering the available load current. To calculate the maximum
output current for a given maximum switch current use the following equation:
C4
1nF
IRIPPLE =
12
×
1
3
×
−5
= 0.375 A
12 + − 5
47 × 10
200 × 10
High ripple currents are present in both the input and output
capacitors, and their ripple current ratings must be large enough
to sustain the large switching currents present in this topology.
The capacitors should have a ripple current rating of at least:
−6
IRMS(CIN, COUT) ≈ IOUT ×
VOUT
(17)
VIN
The peak current seen by the diode, switch, and inductor can be
found by rearranging the load current equation:
The circuit in Figure 6 shows the ADP3050 in a buck-boost
configuration, which produces a negative output voltage from a
positive input voltage. This topology looks quite similar to the
buck shown in Figure 5 above (except the IC and the output filter
are now referenced to the negative output instead of ground), but
REV. A
–15–
VIN + VOUT
 1

IPEAK = 
× IOUT  +  × IRIPPLE 

VIN

 2
(18)
ADP3050
the –5 V supply. The –5 V output would be generated even
without C6 in the circuit, but its inclusion greatly improves the
regulation of the negative output and lowers the inductor ripple
current. The total output current available for both supplies is
limited by the ADP3050 (internally limited to around 1.0 A).
 12 + − 5
 1

IPEAK = 
× 0.5 +  × 0.375 = 0.9 A

12
 2

The average current diode will be equal to the load current.
An inductor with a current rating 20% greater than 0.9 A should
be used (rating of at least 1.2 A). Inductors and diodes with ratings
greater than 1 A should always be used, even if the calculated peak
and average currents are lower. This will ensure that start-up and
fault conditions will not overstress the components.
For the buck-boost topology, the input voltage can be less than
the output voltage (i.e., VIN = 4 V, VOUT = –5 V), but the available load current will be even lower. The equations given in this
section are valid for input voltages less than and greater than the
output voltage. The voltage seen by the ADP3050 is equal to the
sum of the input and output voltages (the BOOST pin sees the
sum of VIN + 2 ⫻ |VOUT|). Make sure that the maximum voltage
ratings of these pins are not exceeded.
Dual Output SEPIC Regulator
For many systems, a dual polarity supply is needed. The circuit
in Figure 7 generates both a positive and a negative 5 V output
using a single magnetic component. The two inductors shown
are actually two separate windings on a single core contained in
a small, surface-mount package. The windings can be connected
in parallel or in series to be used as a single inductor for a conventional buck regulator, or they can be used as a 1:1 transformer,
as in this application. One winding is used as the standard buck
inductor for the +5 V output. The second winding is used to
generate the –5 V output along with D2, C6, and C7.
+ C7
100␮F
ⴚ5V @ 0.25A
VOUT
+
L1*
25␮H
D1
1N5818
C6
100␮F
D2
1N5818
+5V @ 0.5A
VOUT
+ C5
100␮F
D3
1N4148
C3
0.22␮F
*INDUCTOR IS A SINGLE CORE
WITH TWO WINDINGS
COILTRONICS CTX25-4
1
SWITCH
2
BOOST
3
BIAS
4
FB
IN
8
GND
7
SD
6
COMP
5
U1
ADP3050-5
The ripple voltage of the +5 V output is that of a normal buck
regulator (as described in the Applications Information section).
This ripple voltage is determined by the inductor ripple current
and the ESR of the output capacitor. For the system below, the
positive output voltage ripple is a 30 mV peak-to-peak triangular
wave. The ripple voltage of the –5 V output is a rectangular
wave (due to the rectangular shape of the current waveform into
the –5 V output capacitor). The amplitude of this current waveform is approximately equal to twice the –5 V load current. For
a load current of 200 mA and an ESR of 100 mΩ, the negative
output voltage ripple is around 2 ⫻ 200 mA ⫻ 100 mΩ, or
about 40 mV. The edges of this ripple waveform are quite fast,
which, along with the inductance of the output capacitor, generates
narrow spikes on the negative output voltage. These spikes can
easily be filtered out using an additional 5 µF to 10 µF bypass
capacitor close to the load (the inductance of the PC board
trace and the additional capacitor create a low-pass filter to
remove these high frequency spikes).
OUTLINE DIMENSIONS
Dimensions shown in inches and (mm).
8-Lead SOIC
(R Suffix)
0.1968 (5.00)
0.1890 (4.80)
R1
5.1k⍀
C4
1nF
8
0.1574 (4.00)
0.1497 (3.80) 1
SD
12V
VIN
+ C1
22␮F
PIN 1
0.0098 (0.25)
0.0040 (0.10)
C2
0.01␮F
5
4
0.2440 (6.20)
0.2284 (5.80)
0.0688 (1.75)
0.0532 (1.35)
0.0196 (0.50)
x 45°
0.0099 (0.25)
GND
0.0500 0.0192 (0.49)
SEATING (1.27)
0.0098 (0.25)
PLANE BSC 0.0138 (0.35) 0.0075 (0.19)
Figure 7. Dual Output +5 V and –5 V Regulator
8°
0° 0.0500 (1.27)
0.0160 (0.41)
These components form a SEPIC (Single Ended Primary Inductance Converter) using the 1:1 coupled inductor to generate the
negative supply. When the switch is off, the voltage across the buck
winding is equal to VO + VD (VD is the diode drop). This voltage is
generated across the second winding, which is connected to produce
–16–
REV. A
PRINTED IN U.S.A.
L1*
25␮H
Keeping load currents below 500 mA and 250 mA, for the positive and negative supplies, respectively, will ensure that current
limit is not reached under normal operation. These limits are
not interchangeable; 500 mA cannot be drawn from the –5 V
supply while drawing only 250 mA from the +5 V supply. The
maximum current available from the –5 V output is directly related
to the +5 V load current due to the fact that the +5 V output is
used to regulate both supplies. Typically, the –5 V load current
should be around one-half of the +5 V load current to ensure good
regulation of both outputs. Additionally, the –5 V output should
have a preload (the minimum current level) of 1% to 2% of the
+5 V load current. This will help maintain good regulation of the
–5 V output at light loads.
C00125–0–12/00 (rev. A)
The largest peak currents occur at the lowest input voltage. For
this design with a load current of 500 mA: