FEATURES
Initial Accuracy: ⴞ6 mV Max
Low TCV
Load Regulation: 60 ppm/mA
Line Regulation: 25 ppm/V
Wide Operating Range:
2.4 V–18 V for ADR390
2.8 V–18 V for ADR391
Low Power: 120 A Max
Shutdown to Less than 3 A Max
High Output Current: 5 mA Min
Wide Temperature Range: ⴚ40ⴗC to +85ⴗC
Tiny SOT-23-5 Package
APPLICATIONS
Battery-Powered Instrumentation
Portable Medical Instruments
Data Acquisition Systems
Industrial and Process Control Systems
Hard Disk Drives
Automotive
: 25 ppm/ⴗC Max
O
SOT-23 Voltage References with Shutdown
ADR390/ADR391
PIN CONFIGURATION
5-Lead SOT-23
(RT Suffix)
1
SHDN
V
OUT(SENSE)
ADR390/
V
2
IN
ADR391
3
Table I.
Part NumberNominal Output Voltage (V)
ADR3902.048
ADR3912.500
5
GND
4
V
OUT(FORCE)
GENERAL DESCRIPTION
The ADR390 and ADR391 are precision 2.048 V and 2.5 V
bandgap voltage references featuring high accuracy and stability
and low power consumption in a tiny footprint. Patented temperature drift curvature correction techniques minimize nonlinearity of
the voltage change with temperature. The wide operating range
and low power consumption with additional shutdown capability
make them ideal for 3 V to 5 V battery-powered applications. The
Sense Pin enables greater accuracy by supporting full Kelvin
V
OUT
operation in systems using very fine or long circuit traces.
The ADR390 and ADR391 are micropower, Low Dropout Voltage
(LDV) devices that provide a stable output voltage from supplies as
low as 300 mV above the output voltage. They are specified over the
industrial (–40°C to +85°C) temperature range. Each is available
in the tiny 5-lead SOT-23 package.
The combination of V
sense and shutdown functions also
OUT
enables a number of unique applications combining precision
reference/regulation with fault decision and over-current protection. Details are provided in the applications section.
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.
Initial AccuracyV
Initial Accuracy ErrorV
Temperature CoefficientTCV
Minimum Supply Voltage HeadroomV
Line Regulation∆V
Load Regulation∆V
Quiescent CurrentI
Voltage Noisee
Turn-On Settling Timet
Long-Term Stability
Output Voltage Hysteresis
1
2
Ripple Rejection RatioRRRf
Short Circuit to GNDI
Shutdown Supply CurrentI
Shutdown Logic Input CurrentI
Shutdown Logic LowV
Shutdown Logic HighV
NOTES
1
Long-term stability, typical shift in value of output voltage at 25°C on a sample of parts subjected to operation life test of 1000 hours at 125°C. ∆VO = VO (t0) –V
(t
); VO (t0) = VO at 25°C at time 0; VO (t
1000
2
Output Voltage Hysteresis, is defined as the change in 25°C output voltage before and after the device is cycled through temperature. +25 °C to –40°C to +85°C to
+25°C. This is a typical value from a sample of parts put through such a cycle. Refer to Figures 11 and 12. V
at 25°C after temperature cycle at +25°C to –40°C to +85°C to +25°C; V
Specifications subject to change without notice.
1000
O
OERR
/°C–40°C < TA < +85°C525ppm/°C
O
– V
IN
O
/∆V
O
IN
/∆I
O
LOAD
IN
N
R
∆V
O
V
OHYS
SC
SHDN
LOGIC
INL
INH
) = VO at 25°C after 1000 hours at 125°C; ∆VO = (VO (t0) – VO (t
VIN = 2.5 V to 15 V
–40°C < T
V
= 3 V,
IN
I
LOAD
–40°C < T
< +85°C1025ppm/V
A
= 0 mA to 5 mA
< +85°C60ppm/mA
A
No Load100120µA
–40°C < T
< +85°C140µA
A
0.1 Hz to 10 Hz5µV p-p
1,000 Hours50ppm
= 60 Hz85dB
IN
OHYS
= ((VO–V
)/VO) × 106 (in ppm).
OTC
2.0422.048 2.054V
0.290.29%
300mV
20µs
40ppm
30mA
3µA
500nA
0.8V
2.4V
))/VO (t0) × 106 (in ppm).
1000
OHYS
= VO –V
; VO = VO at 25°C at time 0; V
OTC
OTC
O
= V
O
ELECTRICAL CHARACTERISTICS
(@ VIN = 15 V, TA = 25ⴗC unless otherwise noted)
ParameterSymbolConditionsMinTypMaxUnit
Initial AccuracyV
Initial Accuracy ErrorV
Temperature CoefficientTCV
Minimum Supply Voltage HeadroomV
Line Regulation∆V
Load Regulation∆V
Quiescent CurrentI
Voltage Noisee
Turn-On Settling Timet
Long-Term Stability
Output Voltage Hysteresis
1
2
Ripple Rejection RatioRRRf
Short Circuit to GNDI
Shutdown Supply CurrentI
Shutdown Logic Input CurrentI
Shutdown Logic LowV
Shutdown Logic HighV
NOTES
1
Long-term stability, typical shift in value of output voltage at 25°C on a sample of parts subjected to operation life test of 1000 hours at 125°C. ∆VO = VO (t0) –V
(t
); VO (t0) = VO at 25°C at time 0; VO (t
1000
2
Output Voltage Hysteresis, is defined as the change in 25°C output voltage before and after the device is cycled through temperature. +25 °C to –40°C to +85°C to
+25°C. This is a typical value from a sample of parts put through such a cycle. Refer to Figures 11 and 12. V
at 25°C after temperature cycle at +25°C to –40°C to +85°C to +25°C; V
Specifications subject to change without notice.
1000
O
OERR
/°C–40°C < TA < +85°C525ppm/°C
O
– V
IN
O
/∆V
O
IN
/∆I
O
LOAD
IN
N
R
∆V
O
V
OHYS
SC
SHDN
LOGIC
INL
INH
) = VO at 25°C after 1000 hours at 125°C; ∆VO = (VO (t0) – VO (t
VIN = 2.5 V to 15 V
–40°C < T
V
= 3 V,
IN
I
LOAD
–40°C < T
< +85°C1025ppm/V
A
= 0 mA to 5 mA
< +85°C60ppm/mA
A
No Load100120µA
–40°C < T
< +85°C140µA
A
0.1 Hz to 10 Hz5µV p-p
1,000 Hours50ppm
= 60 Hz85dB
IN
OHYS
= ((VO–V
)/VO) × 106 (in ppm).
OTC
2.0422.048 2.054V
0.290.29%
300mV
20µs
40ppm
30mA
3µA
500nA
0.8V
VIN – 1V
))/VO (t0) × 106 (in ppm).
1000
OHYS
= VO –V
; VO = VO at 25°C at time 0; V
OTC
OTC
O
= V
O
–2–
REV. 0
Page 3
ADR391 SPECIFICATIONS
ADR390/ADR391
ELECTRICAL CHARACTERISTICS
(@ VIN = 5 V, TA = 25ⴗC unless otherwise noted)
ParameterSymbolConditionsMinTypMaxUnit
Initial AccuracyV
Initial Accuracy ErrorV
Temperature CoefficientTCV
Minimum Supply Voltage HeadroomV
Line Regulation∆V
Load Regulation∆V
Quiescent CurrentI
Voltage Noisee
Turn-On Settling Timet
Long-Term Stability
Output Voltage Hysteresis
1
2
Ripple Rejection RatioRRRf
Short Circuit to GNDI
Shutdown Supply CurrentI
Shutdown Logic Input CurrentI
Shutdown Logic LowV
Shutdown Logic HighV
NOTES
1
Long-term stability, typical shift in value of output voltage at 25°C on a sample of parts subjected to operation life test of 1000 hours at 125°C. ∆VO = VO (t0) –V
(t
); VO (t0) = VO at 25°C at time 0; VO (t
1000
2
Output Voltage Hysteresis, is defined as the change in 25°C output voltage before and after the device is cycled through temperature. +25 °C to –40°C to +85°C to
+25°C. This is a typical value from a sample of parts put through such a cycle. Refer to Figures 11 and 12. V
at 25°C after temperature cycle at +25°C to –40°C to +85°C to +25°C; V
Specifications subject to change without notice.
1000
O
OERR
/°C–40°C < TA < +85°C525ppm/°C
O
– V
IN
O
/∆V
O
IN
/∆I
O
LOAD
IN
N
R
∆V
O
V
OHYS
SC
SHDN
LOGIC
INL
INH
) = VO at 25°C after 1000 hours at 125°C; ∆VO = (VO (t0) – VO (t
VIN = 2.8 V to 15 V
–40°C < T
V
= 3.5 V,
IN
I
LOAD
–40°C < T
< +85°C1025ppm/V
A
= 0 mA to 5 mA
< +85°C60ppm/mA
A
No Load100120µA
–40°C < T
< +85°C140µA
A
0.1 Hz to 10 Hz5µV p-p
1,000 Hours50ppm
= 60 Hz85dB
IN
OHYS
= ((VO–V
)/VO) × 106 (in ppm).
OTC
2.4942.52.506V
0.240.24%
300mV
20µs
75ppm
25mA
3µA
500nA
0.8V
2.4V
))/VO (t0) × 106 (in ppm).
1000
OHYS
= VO –V
; VO = VO at 25°C at time 0; V
OTC
OTC
O
= V
O
ELECTRICAL CHARACTERISTICS
(@ VIN = 15 V, TA = 25ⴗC unless otherwise noted)
ParameterSymbolConditionsMinTypMaxUnit
Initial AccuracyV
Initial Accuracy ErrorV
Temperature CoefficientTCV
Minimum Supply Voltage HeadroomV
Line Regulation∆V
Load Regulation∆V
Quiescent CurrentI
Voltage Noisee
Turn-On Settling Timet
Long-Term Stability
Output Voltage Hysteresis
1
2
Ripple Rejection RatioRRRf
Short Circuit to GNDI
Shutdown Supply CurrentI
Shutdown Logic Input CurrentI
Shutdown Logic LowV
Shutdown Logic HighV
NOTES
1
Long-term stability, typical shift in value of output voltage at 25°C on a sample of parts subjected to operation life test of 1000 hours at 125°C. ∆VO = VO (t0) –V
(t
); VO (t0) = VO at 25°C at time 0; VO (t
1000
2
Output Voltage Hysteresis, is defined as the change in 25°C output voltage before and after the device is cycled through temperature. +25 °C to –40°C to +85°C to
+25°C. This is a typical value from a sample of parts put through such a cycle. Refer to Figures 11 and 12. V
at 25°C after temperature cycle at +25°C to –40°C to +85°C to +25°C; V
Specifications subject to change without notice.
1000
O
OERR
/°C–40°C < TA < +85°C525ppm/°C
O
– V
IN
O
/∆V
O
IN
/∆I
O
LOAD
IN
N
R
∆V
O
V
OHYS
SC
SHDN
LOGIC
INL
INH
) = VO at 25°C after 1000 hours at 125°C; ∆VO = (VO (t0) – VO (t
Lead Temperature Range (Soldering, 60 sec) . . . . . . . . 300°C
*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 rating conditions for extended periods may affect device reliability.
ORDERING GUIDE
TemperaturePackagePackageTopOutputNumber of
ModelRangeDescriptionOptionMarkVoltageParts
ADR390ART–REEL7–40⬚C to +85⬚C5-Lead SOTRT-5R0A2.0483,000
ADR390ART–REEL–40⬚C to +85⬚C5-Lead SOTRT-5R0A2.04810,000
ADR391ART–REEL7–40⬚C to +85⬚C5-Lead SOTRT-5R1A2.5003,000
ADR391ART–REEL–40⬚C to +85⬚C5-Lead SOTRT-5R1A2.50010,000
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 ADR390/ADR391 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.
–4–
REV. 0
Page 5
Typical Performance Characteristics–
ADR390/ADR391
– V
OUT
V
2.054
2.052
2.050
2.048
2.046
2.044
2.042
SAMPLE 1
SAMPLE 2
SAMPLE 3
ⴚ40ⴚ15
10356085
TEMPERATURE – ⴗC
Figure 1. ADR390 Output Voltage vs. Temperature
2.506
– V
OUT
V
2.504
2.502
2.500
2.498
2.496
SAMPLE 1
SAMPLE 2
SAMPLE 3
140
120
100
80
SUPPLY CURRENT – A
60
40
2.515.05.0
+85ⴗC
+25ⴗC
ⴚ40ⴗC
7.510.012.5
INPUT VOLTAGE – V
Figure 4. ADR391 Supply Current vs. Input Voltage
40
IL= 0mA TO 5mA
35
30
25
20
LOAD REGULATION – ppm/mA
15
VIN = 3.0V
VIN = 5.0V
2.494
ⴚ40ⴚ15
10356085
TEMPERATURE – ⴗC
Figure 2. ADR391 Output Voltage vs. Temperature
140
120
100
80
SUPPLY CURRENT – A
60
40
2.515.05.0
+85ⴗC
+25ⴗC
ⴚ40ⴗC
7.510.012.5
INPUT VOLTAGE – V
Figure 3. ADR390 Supply Current vs. Input Voltage
10
ⴚ40ⴚ15
10356085
TEMPERATURE – ⴗC
Figure 5. ADR390 Load Regulation vs. Temperature
40
IL= 0mA TO 5mA
35
30
25
20
LOAD REGULATION – ppm/mA
15
10
ⴚ40ⴚ15
VIN = 3.5V
VIN = 5.0V
10356085
TEMPERATURE – ⴗC
Figure 6. ADR391 Load Regulation vs. Temperature
–5–REV. 0
Page 6
ADR390/ADR391
5
VIN = 2.5V TO 15V
4
3
2
LINE REGULATION – ppm/V
1
0
ⴚ40ⴚ15
10356085
TEMPERATURE – ⴗC
Figure 7. ADR390 Line Regulation vs. Temperature
5
VIN = 2.8V TO 15V
4
3
2
LINE REGULATION – ppm/V
1
0.8
0.6
+85ⴗC
0.4
0.2
DIFFERENTIAL VOLTAGE – V
0
0
234
LOAD CURRENT – mA
+25ⴗC
ⴚ40ⴗC
51
Figure 10. ADR391 Minimum Input-Output Voltage
Differential vs. Load Current
60
TEMPERATURE: +25ⴗC ⴚ40ⴗC +85ⴗC +25ⴗC
50
40
30
FREQUENCY
20
10
0
ⴚ40ⴚ15
10356085
TEMPERATURE – ⴗC
Figure 8. ADR391 Line Regulation vs. Temperature
0.8
0.6
0.4
0.2
DIFFERENTIAL VOLTAGE – V
0
0
ⴚ40ⴗC
+85ⴗC
+25ⴗC
234
LOAD CURRENT – mA
51
Figure 9. ADR390 Minimum Input-Output Voltage
Differential vs. Load Current
0
ⴚ0.24
Figure 11. ADR390 V
70
60
50
40
30
FREQUENCY
20
10
0
ⴚ0.56ⴚ0.26
Figure 12. ADR391 V
ⴚ0.12
ⴚ0.18ⴚ0.06
TEMPERATURE: +25ⴗC ⴚ40ⴗC +85ⴗC +25ⴗC
ⴚ0.41ⴚ0.11
00.060.18
V
DEVIATION – mV
OUT
Hysteresis Distribution
OUT
V
DEVIATION – mV
OUT
Hysteresis Distribution
OUT
0.120.24
0.040.19
0.30
0.34
–6–
REV. 0
Page 7
ADR390/ADR391
VOLTAGE
TIME – 10s/DIV
0
0
0
0
0
0
0
0
0
C
BYPASS
= 0.1F
LINE
INTERRUPTION
V
OUT
0.5V/DIV
1V/DIV
VOLTAGE – 1V/DIV
TIME – 200s/DIV
0
0
0
0
0
0
0
0
0
CL = 0nF
V
LOAD
ON
V
OUT
LOAD OFF
1k
VIN = 5V
ADR391
ADR390
VOLTAGE NOISE DENSITY – nV/ Hz
100
1010k100
FREQUENCY – Hz
1k
Figure 13. Voltage Noise Density vs. Frequency
0
0
0
0
0
0
0
0
LINE
INTERRUPTION
0
0
VOLTAGE
0
0
0
V
OUT
TIME – 10s/DIV
C
BYPASS
= 0F
0.5V/DIV
1V/DIV
Figure 16. ADR391 Line Transient Response
0
VOLTAGE – 100V/DIV
0
0
0
TIME – 10ms/DIV
Figure 14. ADR390 Voltage Noise 10 Hz to 10 kHz
0
0
0
0
0
0
VOLTAGE – 100V/DIV
0
0
0
Figure 15. ADR391 Voltage Noise 10 Hz to 10 kHz
TIME – 10ms/DIV
Figure 17. ADR391 Line Transient Response
Figure 18. ADR391 Load Transient Response
–7–REV. 0
Page 8
ADR390/ADR391
0
0
0
0
0
0
VOLTAGE – 1V/DIV
0
0
0
V
LOAD
V
OUT
LOAD OFF
ON
TIME – 200s/DIV
CL = 1nF
Figure 19. ADR391 Load Transient Response
0
0
0
0
0
0
VOLTAGE – 1V/DIV
0
V
LOAD
V
OUT
LOAD OFF
ON
CL = 100nF
0
V
= 15V
IN
0
0
0
0
VOLTAGE
V
0
0
0
0
V
IN
OUT
5V/DIV
2V/DIV
TIME – 40s/DIV
Figure 22. ADR391 Turn-Off Response at 15 V
0
C
= 0.1F
BYPASS
0
0
V
0
0
VOLTAGE
0
0
V
OUT
IN
2V/DIV
5V/DIV
0
0
TIME – 200s/DIV
Figure 20. ADR391 Load Transient Response
0
V
= 15V
IN
0
0
0
0
VOLTAGE
0
V
0
0
0
V
OUT
IN
5V/DIV
2V/DIV
TIME – 20s/DIV
Figure 21. ADR391 Turn-On Response Time at 15 V
0
0
TIME – 200s/DIV
Figure 23. ADR391 Turn-On/Turn-Off Response at 5 V
0
RL = 500⍀
0
0
V
0
0
VOLTAGE
0
0
0
0
V
OUT
IN
2V/DIV
5V/DIV
TIME – 200s/DIV
Figure 24. ADR391 Turn-On/Turn-Off Response at 5 V
–8–
REV. 0
Page 9
ADR390/ADR391
SHDN
FORCE
SENSE
V
IN
R59 R44
TESTPAD
R58
R53
R54
R49
TESTPAD
R48
GROUND
R61
R60
Q51
Q52
2RS
TESTPAD
0
RL = 500⍀
0
= 100nF
C
L
0
0
0
0
VOLTAGE – 5V/DIV
0
0
0
V
OUT
V
IN
2V/DIV
5V/DIV
TIME – 200s/DIV
Figure 25. ADR391 Turn-On/Turn-Off Response at 5 V
80
60
40
20
0
ⴚ20
ⴚ40
ⴚ60
RIPPLE REJECTION – dB
ⴚ80
ⴚ100
ⴚ120
101M100
1k10k100k
FREQUENCY – Hz
Figure 26. Ripple Rejection vs. Frequency
100
90
80
70
60
50
40
30
OUTPUT IMPEDANCE – ⍀
20
10
0
101M100
Figure 27. Output Impedance vs. Frequency
CL = 1F
1k10k100k
FREQUENCY – Hz
CL = 0F
CL = 0.1F
THEORY OF OPERATION
Bandgap references are the high-performance solution for low
supply voltage and low power voltage reference applications,
and the ADR390/ADR391 is no exception. But the uniqueness
of this product lies in its architecture. By observing Figure 28,
the zero TC bandgap voltage is referenced to the output, not to
ground. The bandgap cell consists of the pnp pair Q51 and Q52,
running at unequal current densities. The difference in V
BE
results in a voltage with a positive TC which is amplified up by
58
R
2
×
the ratio of
. This PTAT voltage, combined with VBE’s
54
R
of Q51 and Q52 produce the stable bandgap voltage.
Reduction in the bandgap curvature is performed by the ratio of
the two resistors R44 and R59. Precision laser trimming and
other patented circuit techniques are used to further enhance
the drift performance.
Figure 28. Simplified Schematic
Device Power Dissipation Considerations
The ADR390/ADR391 is capable of delivering load currents to
5 mA with an input voltage that ranges from 2.8 V (ADR391 only)
to 15 V. When this device is used in applications with large input
voltages, care should be taken to avoid exceeding the specified maximum power dissipation or junction temperature that could result in
premature device failure. The following formula should be used to
calculate a device’s maximum junction temperature or dissipation:
TT
−
J
P
=
D
A
θ
JA
In this equation, TJ and TA are, respectively, the junction and
ambient temperatures, P
θ
is the device package thermal resistance.
JA
is the device power dissipation, and
D
Shutdown Mode Operation
The ADR390/ADR391 includes a shutdown feature that is TTL/
CMOS level compatible. A logic LOW or a zero volt condition on
the SHDN pin is required to turn the device off. During shutdown,
the output of the reference becomes a high impedance state where
its potential would then be determined by external circuitry. If the
shutdown feature is not used, the SHDN pin should be connected
(Pin 2).
to V
IN
–9–REV. 0
Page 10
ADR390/ADR391
U1
ADR39x
R1
4.99k⍀
(SEE TEXT)
C1
0.1F
V
IN
VIN > V
OUT2
+0.15V
V
IN
COMMON
V
OUT
COMMON
1
2
4
5
V
OUT2
3.735V
VO (U1)
C2
1F
D1
AD589
VO (D1)
C3
1F
V
OUT1
1.235V
5V
APPLICATIONS
Membrane Switch Controlled Power Supply
The ADR390/ADR391 can operate as a low dropout power
supply in hand-held instrumentation. In the following circuit, a
membrane ON/OFF switch is used to control the operation of the
reference. During an initial power-on condition, the SHDN pin is
held to GND. Recall that this condition disables the output (read:
three-state). When the membrane ON switch is pressed, the SHDN
pin assumes and remains at the same potential as V
, via the 10 kΩ
IN
resistor thus enabling the output. When the membrane OFF switch
is pressed, the SHDN pin is momentarily connected to GND which
disables the ADR390/ADR391 output once again.
V
IN
10k⍀
ON
OFF
ADR39x
1F
TANT
V
OUT
Figure 29. Membrane Switch Controlled Power Supply
Stacking Reference ICs for Arbitrary Outputs
Some applications may require two reference voltage sources which
are a combined sum of standard outputs. The following circuit
shows how this “stacked output” reference can be implemented:
U2, either the external load of U1 or R1 must provide a path for
this current. If the U1 minimum load is not well defined, the
resistor R1 should be used, set to a value that will conservatively
pass 600 µA of current with the applicable V
across it. Note
OUT1
that the two U1 and U2 reference circuits are locally treated as
macrocells, each having its own bypasses at input and output for best
stability. Both U1 and U2 in this circuit can source dc currents up to
their full rating. The minimum input voltage, VS, is determined by
the sum of the outputs, V
, plus the dropout voltage of U2.
OUT2
A related variation on stacking two three-terminal references is
shown in the following figure where U1, an ADR391, is stacked
with a two-terminal reference diode such as the AD589. Similar
to the all three-terminal stacked references mentioned earlier,
the two individual terminal voltage outputs of D1 and U1 are
1.235 V and 2.5 V, respectively. Thus V
is the sum of D1 and
OUT2
U1, or 3.735 V. When using two-terminal reference diodes such
as D1, the rated minimum and maximum device currents must
be observed, and the maximum load current from V
be no greater than the current set up by R1 and V
OUT1
O(U1)
can
.
OUTPUT TABLE
VIN > V
COMMON
V
OUT2
IN
V
IN
+0.15V
0.1F
0.1F
U1/U2
ADR390/ADR390
ADR391/ADR391
C1
C3
U2
1
ADR39x
(SEE TABLE)
U1
1
ADR39x
(SEE TABLE)
2
4
VO (U2)
5
2
4
VO (U1)
5
C2
1F
C4
1F
V
OUT1
2.048
2.5
R1
3.9k⍀
(SEE TEXT)
Figure 30. Stacking Voltage References with the ADR390/
ADR391
Two reference ICs are used, fed from a common unregulated
input, V
in series which provides two output voltages V
V
OUT1
voltage and the terminal voltage of U2. U1 and U2 are simply
chosen for the two voltages that supply the required outputs (see
Output Table). For example, if both U1 and U2 are ADR391’s,
V
OUT1
While this concept is simple, a precaution is in order. Since the
lower reference circuit must sink a small bias current from U2,
plus the base current from the series PNP output transistor in
. The outputs of the individual ICs are simply connected
IN
is the terminal voltage of U1, while V
is 2.5 V and V
OUT2
is 5.0 V.
OUT2
and V
OUT1
is the sum of this
(V)
V
OUT2
4.096
5.0
V
OUT2
V
OUT1
V
OUT
COMMON
OUT2
(V)
Figure 31. Stacking Voltage References with the ADR390/
ADR391
A Negative Precision Reference without Precision Resistors
In many current-output CMOS DAC applications where the
output signal voltage must be of the same polarity as the reference
voltage, it is often required to reconfigure a current-switching
DAC into a voltage-switching DAC through the use of a 1.25 V
reference, an op amp, and a pair of resistors. Using a currentswitching DAC directly requires the need for an additional
operational amplifier at the output to reinvert the signal. A negative
voltage reference is then desirable from the point that an additional
operational amplifier is not required for either reinversion (currentswitching mode) or amplification (voltage switching mode) of the
DAC output voltage. In general, any positive voltage reference can
be converted into a negative voltage reference through the use of an
operational amplifier and a pair of matched resistors in an inverting
configuration. The disadvantage to this approach is that the largest
single source of error in the circuit is the relative matching of the
resistors used.
.
The following circuit avoids the need for tightly matched resistors with the use of an active integrator circuit. In this circuit,
the output of the voltage reference provides the input drive for
the integrator. The integrator, to maintain circuit equilibrium,
adjusts its output to establish the proper relationship between
the reference’s V
and GND. Thus, any negative output
OUT
voltage desired can be chosen by simply substituting for the
appropriate reference IC. The shutdown feature is maintained
in the circuit with the simple addition of a PNP transistor and
–10–
REV. 0
Page 11
ADR390/ADR391
a 10 kΩ resistor. A precaution should be noted with this approach:
although rail-to-rail output amplifiers work best in the application,
these operational amplifiers require a finite amount (mV) of headroom when required to provide any load current. The choice for
the circuit’s negative supply should take this issue into account.
V
IN
10k⍀
SHDN
TTL/CMOS
10k⍀
2N3906
1
SHDN
ADR39x
2
V
GND
5
V
OUT
S
V
OUT
100k⍀
1k⍀
4
1F
1F
+5V
A1
ⴚ5V
A1 = 1/2 OP295,
1/2 OP291
100⍀
ⴚV
REF
Figure 32. A Negative Precision Voltage Reference Uses
No Precision Resistors
Precision Current Source
Many times in low-power applications, the need arises for a precision current source that can operate on low supply voltages. As
shown in the following figure, the ADR390/ADR391 can be configured as a precision current source. The circuit configuration illustrated is a floating current source with a grounded load. The
reference’s output voltage is bootstrapped across R
, which sets
SET
the output current into the load. With this configuration, circuit
precision is maintained for load currents in the range from the
reference’s supply current, typically 90 µA to approximately 5 mA.
V
IN
SHDN
V
OUT
ADR39x
V
V
OUT
S
R
1
R
1
GND
1F
I
ADJUST
R
SY
I
OUT
}
P
1
SET
High-Power Performance with Current Limit
In some cases, the user may want higher output current delivered
to a load and still achieve better than 0.5% accuracy out of the
ADR390/ADR391. The accuracy for a reference is normally
specified on the data sheet with no load. However, the output
voltage changes with load current.
The circuit below provides high current without compromising
the accuracy of the ADR390/ADR391. The series pass transistor Q1 provides up to 1 A load current. The ADR390/ADR391
delivers only the base drive to Q1 through the force pin. The
sense pin of the ADR390/ADR391 is a regulated output and is
connected to the load.
R1
4.7k⍀
V
IN
U1
GND
SHDN
V
IN
V
OUT (FORCE)
V
OUT (SENSE)
ADR390/ADR391
Q2N2222
Q1
R
R
S
L
Q2N4921
I
L
Q2
Figure 34. ADR390/ADR391 for High-Power Performance
with Current Limit
A similar circuit function can also be achieved with the Darlington
transistor configuration, see Figure 35.
R1
4.7k⍀
V
IN
U1
GND
SHDN
V
IN
V
OUT (FORCE)
V
OUT (SENSE)
ADR390/ADR391
Q2N2222
R
Q1
Q2
Q2N4921
S
R
L
R
L
Figure 33. A Precision Current Source
Figure 35. ADR390/ADR391 High Output Current with
Darlington Drive Configuration
The transistor Q2 protects Q1 during short circuit limit faults by
robbing its base drive. The maximum current is I
≈ 0.6 V/RS.
LMAX
–11–REV. 0
Page 12
ADR390/ADR391
0.0669 (1.70)
0.0590 (1.50)
0.0512 (1.30)
0.0354 (0.90)
0.0059 (0.15)
0.0019 (0.05)
OUTLINE DIMENSIONS
Dimensions shown in inches and (mm).
5-Lead SOT-23
(RT Suffix)
0.1181 (3.00)
0.1102 (2.80)
4 5
0.1181 (3.00)
0.1024 (2.60)
0.0374 (0.95) BSC
0.0571 (1.45)
0.0374 (0.95)
SEATING
PLANE
PIN 1
1 3
2
0.0748 (1.90)
BSC
0.0197 (0.50)
0.0138 (0.35)
10ⴗ
0ⴗ
C3863–8–4/00 (rev. 0) 00419
0.0079 (0.20)
0.0031 (0.08)
0.0217 (0.55)
0.0138 (0.35)
–12–
PRINTED IN U.S.A.
REV. 0
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