FEATURES
Enhanced Replacement for LF441 and TL061
DC Performance:
200 A max Quiescent Current
10 pA max Bias Current, Warmed Up (AD548C)
250 V max Offset Voltage (AD548C)
2 V/C max Drift (AD548C)
2 V p-p Noise, 0.1 Hz to 10 Hz
AC Performance:
1.8 V/s Slew Rate
1 MHz Unity Gain Bandwidth
Available in Plastic and Hermetic Metal Can Packages
and in Chip Form
Available in Tape and Reel in Accordance with
EIA-481A Standard
MIL-STD-883B Parts Available
Dual Version Available: AD648
Surface-Mount (SOIC) Package Available
PRODUCT DESCRIPTION
The AD548 is a low power, precision monolithic operational
amplifier. It offers both low bias current (10 pA max, warmed
up) and low quiescent current (200 µA max) and is fabricated
with ion-implanted FET and laser wafer trimming technologies.
Input bias current is guaranteed over the AD548’s entire
common-mode voltage range.
The economical J grade has a maximum guaranteed input offset
voltage of less than 2 mV and an input offset voltage drift of less
than 20 µV/°C. This level of dc precision is achieved utilizing
Analog’s laser wafer drift trimming process. The combination of
low quiescent current and low offset voltage drift minimizes
changes in input offset voltage due to self-heating effects.
The AD548 is recommended for any dual supply op amp application requiring low power and excellent dc and ac performance.
In applications such as battery-powered, precision instrument
front ends and CMOS DAC buffers, the AD548’s excellent combination of low input offset voltage and drift, low bias current,
and low 1/f noise reduces output errors. High common-mode
rejection (82 dB, min on the “B” grade) and high open-loop
gain ensures better than 12-bit linearity in high impedance,
buffer applications.
The AD548 is pinned out in a standard op amp configuration
and is available in three performance grades. The AD548J and
AD548K are rated over the commercial temperature range of
0°C to 70°C. The AD548B is rated over the industrial temperature range of –40°C to +85°C.
The AD548 is available in an 8-lead plastic mini-DIP and
surface-mount (SOIC) packages.
BiFET Op Amp
AD548
CONNECTION DIAGRAMS
Plastic Mini-DIP (N) Package
and
SOIC (R)Package
OFFSET NULL
INVERTING
NONINVERTING
NOTE: PIN 4 CONNECTED TO CASE
NC = NO CONNECT
PRODUCT HIGHLIGHTS
INPUT
INPUT
V–
1
2
3
4
1
AD548
TOP VIEW
10k
VOS TRIM
TOP VIEW
1. A combination of low supply current, excellent dc and ac
performance and low drift makes the AD548 the ideal op
amp for high performance, low power applications.
2. The AD548 is pin compatible with industry standard op
amps such as the LF441, TL061, and AD542, enabling
designers to improve performance while achieving a reduction
in power dissipation of up to 85%.
3. Guaranteed low input offset voltage (2 mV max) and drift
(20 µV/°C max) for the AD548J are achieved utilizing
Analog Devices’ laser drift trimming technology, eliminating
the need for external trimming.
4. Analog Devices specifies each device in the warmed-up
condition, insuring that the device will meet its published
specifications in actual use.
5. A dual version, the AD648, is also available.
6. Enhanced replacement for LF441 and TL061.
8
7
6
5
5
–15V
4
NC
V+
OUTPUT
OFFSET
NULL
REV. C
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 that
may result from its use. No license is granted by implication or otherwise
under any patent or patent rights of Analog Devices.
Commercial (0°C to 70°C)AD548JAD548K
Industrial (–40°C to +85°C)AD548AAD548B
Military (–55°C to +125°C)AD548S
PACKAGE OPTIONS
SOIC (R-8)AD548JRAD548KR
Plastic (N-8)AD548JN
4
AD548KN
Tape and ReelAD548JR-REELAD548KR-REEL
NOTES
1
Input Offset Voltage specifications are guaranteed after five minutes of operation at TA = 25°C.
2
Bias Current specifications are guaranteed maximum at either input after five minutes of operation at TA = 25°C. For higher temperature, the current doubles every 10°C.
3
Defined as voltages between inputs, such that neither exceeds ±10 V from ground.
4
Not recommended for new designs; obsolete April 2002.
Storage Temperature Range (Q, H) . . . . . . . –65°C to +150°C
(N, R) . . . . . . . . –65°C to +125°C
NOTES
1
Stresses above those listed under Absolute Maximum Ratings may cause
permanent damage to the device. This is a stress rating only; functional operation
of the device at these or any other conditions above those indicated in the
operational sections of this specification is not implied. Exposure to absolute
maximum rating conditions for extended periods may affect device reliability.
Lead Temperature Range (Soldering 60 sec) . . . . . . . . . 300°C
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 AD548 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.
= 42°C/W;
JC
–4–
REV. C
Typical Performance Characteristics–
AD548
20
15
+V
IN
10
–V
IN
INPUT VOLTAGE – ±V
5
0
0 5 10 15 20
SUPPLY VOLTAGE – V
TPC 1. Input Voltage Range
vs. Supply Voltage
200
180
160
140
QUIESCENT CURRENT – µA
20
15
10
5
OUTPUT VOLTAGE SWING – ±V
0
0 5 10 15 20
SUPPLY VOLTAGE – V
TPC 2. Output Voltage Swing
vs. Supply Voltage
10
8
6
4
INPUT BIAS CURRENT – pA
2
+V
OUT
–V
OUT
25°C
RL = 10k
30
25
20
15
10
5
OUTPUT VOLTAGE SWING – V p-p
0
10 100 1k 10k
LOAD RESISTANCE –
TPC 3. Output Voltage Swing
vs. Load Resistance
100nA
10nA
1nA
100pA
10pA
1pA
INPUT BIAS CURRENT
100fA
120
0 5 10 15 20
SUPPLY VOLTAGE – V
TPC 4. Quiescent Current vs.
Supply Voltage
10
8
6
4
INPUT BIAS CURRENT – pA
2
0
–10 –6 –2 2 6 10
COMMON-MODE VOLTAGE – V
TPC 7. Input Bias Current vs.
Common-Mode Voltage
0
0 4 8 12 16 20
SUPPLY VOLTAGE – V
TPC 5. Input Bias Current
vs. Supply Voltage
30
25
20
I – V
15
OS
I∆V
10
5
0
0 10 20 30 40 50 60 70
WARM-UP TIME – Sec
TPC 8. Change in Offset Voltage
vs. Warm-Up Time
10fA
–55 –25 5 35 65 95 125
TEMPERATURE – °C
TPC 6. Input Bias Current vs.
Temperature
1500
1250
1000
750
500
OPEN LOOP GAIN – V/mV
250
0
–55 –25 5 35 65 95 125
TEMPERATURE – °C
RL = 10k
TPC 9. Open-Loop Gain vs.
Temperature
REV. C
–5–
AD548
100
80
60
40
20
0
OPEN LOOP GAIN – dB
–20
–40
1k 10k 100k 1M 10M
PHASE
GAIN
FREQUENCY – Hz
TPC 10. Open-Loop Frequency
Response
90
80
70
60
50
CMRR – dB
40
30
20
1k 10k 100k 1M
FREQUENCY – Hz
TPC 13. CMRR vs. Frequency
100
80
60
40
20
PHASE IN DEGREES
0
–20
–40
120
110
100
90
80
70
OPEN LOOP VOLTAGE GAIN – dB
60
0 2 4 6 8 10 12 14 16 18
SUPPLY VOLTAGE – V
TPC 11. Open-Loop Voltage Gain
vs. Supply Voltage
22
20
18
16
14
12
10
8
6
OUTPUT VOLTAGE – V p-p
4
2
0
10 100 1k 10k 100k 1M
FREQUENCY – Hz
TPC 14. Large Signal Frequency
Response
120
100
80
60
40
20
0
POWER SUPPLY REJECTION – dB
–20
100 1k 10k 100k 1M
+SUPPLY
–SUPPLY
FREQUENCY – Hz
TPC 12. PSRR vs. Frequency
10
5
0
–5
OUTPUT VOLTAGE SWING – V
–10
0 2 4 6 8
10mV
1mV
1mV
10mV
SETTLING TIME – µs
TPC 15. Output Swing and Error
Voltage vs. Output Settling Time
4
1
FOLLOWER
WITH GAIN = 10
0.1
0.01
TOTAL HARMONIC DISTORTION – %
0.001
100 1k 10k
UNITY GAIN
FOLLOWER
FREQUENCY – Hz
TPC 16. Total Harmonic
Distortion vs. Frequency
100k
160
140
120
100
80
60
40
INPUT NOISE VOLTAGE – nV/√Hz
20
0
10 100 1k 10k 100k
FREQUENCY – Hz
TPC 17. Input Noise Voltage
Spectral Density
–6–
WHENEVER JOHNSON NOISE IS GREATER THAN
AMPLIFIER NOISE, AMPLIFIER NOISE CAN BE
CONSIDERED NEGLIGIBLE FOR APPLICATION
10,000
1,000
INPUT NOISE VOLTAGE – µV p-p
RESISTOR JOHNSON
100
10
1
0
100k 1M 10M 100M 1G 10G 100G
1kHz BANDWIDTH
NOISE
10Hz
BANDWIDTH
AMPLIFIER GENERATED NOISE
SOURCE IMPEDANCE –
TPC 18. Total Noise vs. Source
Impedance
REV. C
AD548
TPC 19a. Unity Gain Follower
TPC 20a. Utility Gain Inverter
APPLICATION NOTES
TPC 19b. Unity Gain Follower
Pulse Response (Large Signal)
TPC 20b. Utility Gain Inverter
Pulse Response (Large Signal)
The AD548 is a JFET-input op amp with a guaranteed maximum I
of less than 10 pA, and offset and drift laser-trimmed to
B
0.5 mV and 5 µV/°C, respectively (AD548B). AC specs include
1 MHz bandwidth, 1.8 V/µs typical slew rate and 8 µs settling time
for a 20 V step to ±0.01%—all at a supply current less than
200 µA. To capitalize on the device’s performance, a number of
error sources should be considered.
The minimal power drain and low offset drift of the AD548
reduce self-heating or “warm-up” effects on input offset voltage,
making the AD548 ideal for on/off battery-powered applications. The power dissipation due to the AD548’s 200 µA supply
current has a negligible effect on input current, but heavy output loading will raise the chip temperature. Since a JFET’s
input current doubles for every 10°C rise in chip temperature,
this can be a noticeable effect.
The amplifier is designed to be functional with power supply
voltages as low as ±4.5 V. It will exhibit a higher input offset
voltage than at the rated supply voltage of ±15 V, due to power
supply rejection effects. The common-mode range of the AD548
extends from 3 V more positive than the negative supply to 1 V
more negative than the positive supply. Designed to cleanly
drive up to 10 kΩ and 100 pF loads, the AD548 will drive a 2
kΩ load with reduced open-loop gain.
OFFSET NULLING
Unlike bipolar input amplifiers, zeroing the input offset voltage
of a BiFET op amp will not minimize offset drift. Using balance
Pins 1 and 5 to adjust the input offset voltage as shown in
Figure 1 will induce an added drift of 0.24 µV/°C per 100 µV of
nulled offset. The low initial offset (0.5 mV) of the AD548B
results in only 0.6 µV/°C of additional drift.
TPC 19c. Unity Gain Follower
Pulse Response (Small Signal)
TPC 20c. Unity Gain Inverter
Pulse Response (Small Signal)
Figure 1. Offset Null Configuration
LAYOUT
To take full advantage of the AD548’s 10 pA max input current,
parasitic leakages must be kept below an acceptable level. The
practical limit of the resistance of epoxy or phenolic circuit
board material is between 1 × 10
result in an additional leakage of 5 pA between an input of 0 V
and a –15 V supply line. Teflon
rial (with a resistance exceeding 10
12
Ω and 3 × 10
®
or a similar low leakage mate-
17
Ω) should be used to
12
Ω. This can
isolate high impedance input lines from adjacent lines carrying
high voltages. The insulator should be kept clean, since contaminants will degrade the surface resistance.
A metal guard completely surrounding the high impedance nodes
and driven by a voltage near the common-mode input potential
can also be used to reduce some parasitic leakages. The guarding
pattern in Figure 2 will reduce parasitic leakage due to finite
board surface resistance; but it will not compensate for a low
volume resistivity board.
Teflon is a registered trademark of DuPont.
REV. C
–7–
AD548
Figure 2. Board Layout for Guarding Inputs
INPUT PROTECTION
The AD548 is guaranteed to withstand input voltages equal to
the power supply potential. Exceeding the negative supply voltage on either input will forward bias the substrate junction of
the chip. The induced current may destroy the amplifier due to
excess heat.
Input protection is required in applications such as a flame
detector in a gas chromatograph, where a very high potential
may be applied to the input terminals during a sensor fault
condition. Figure 3 shows a simple current limiting scheme that
can be used. R
PROTECT
mum overload current is 1.0 mA (l00 kΩ for a 100 V overload,
for example).
Exceeding the negative common-mode range on either input
terminal causes a phase reversal at the output, forcing the
amplifier output to the corresponding high or low state. Exceeding the negative common-mode on both inputs simultaneously
forces the output high. Exceeding the positive common-mode
range on a single input does not cause a phase reversal, but if
both inputs exceed the limit the output will be forced high. In
all cases, normal amplifier operation is resumed when input
voltages are brought back within the common-mode range.
should be chosen such that the maxi-
Figure 4. AD548 Used as DAC Output Amplifier
That is:
VOSOutput =VOSInput 1+
R
FB
R
O
RFB is the feedback resistor for the op amp, which is internal to
the DAC. R
value of R
is the DAC’s R-2R ladder output resistance. The
O
is code dependent. This has the effect of changing
O
the offset error voltage at the amplifier’s output. An output
amplifier with a sub millivolt input offset voltage is needed to
preserve the linearity of the DAC’s transfer function.
The AD548 in this configuration provides a 700 kHz small
signal bandwidth and 1.8 V/µs typical slew rate. The 33 pF
capacitor across the feedback resistor optimizes the circuit’s
response. The oscilloscope charts in Figures 5 and 6 show small
and large signal outputs of the circuit in Figure 4. Upper traces
show the input signal V
. Lower traces are the resulting output
IN
voltage with the DAC’s digital input set to all 1s. The AD548
settles to ±0.01% for a 20 V input step in 14 µs.
5V 5µS 20V
100
90
Figure 3. Input Protection of IV Converter
D/A CONVERTER OUTPUT BUFFER
The circuit in Figure 4 shows the AD548 and AD7545 12-bit
CMOS D/A converter in a unipolar binary configuration. V
will be equal to V
digital word. V
adjusting R
IN
attenuated by a factor depending on the
REF
sets the full scale. Overall gain is trimmed by
REF
. The AD548’s low input offset voltage, low drift,
OUT
and clean dynamics make it an attractive low power output buffer.
The input offset voltage of the AD548 output amplifier results
in an output error voltage. This error voltage equals the input
offset voltage of the op amp times the noise gain of the amplifier.
–8–
10
0%
Figure 5. Response to ±20 V p-p Reference Square Wave
50mV
100
90
10
0%
2µS 200mV
Figure 6. Response to ±100 mV p-p Reference Square Wave
REV. C
PHOTODIODE PREAMP
The performance of the photodiode preamp shown in Figure 7
is enhanced by the AD548’s low input current, input voltage
offset, and offset voltage drift. The photodiode sources a current
proportional to the incident light power on its surface. R
the photodiode current to an output voltage equal to R
converts
F
× IS.
F
Figure 7.
An error budget illustrating the importance of low amplifier
input current, voltage offset, and offset voltage drift to minimize
output voltage errors can be developed by considering the equivalent circuit for the small (0.2 mm
2
area) photodiode shown in
Figure 7. The input current results in an error proportional to
the feedback resistance used. The amplifier’s offset will produce
an error proportional to the preamp’s noise gain (I + R
where R
is the photodiode shunt resistance. The amplifier’s
SH
F/RSH
),
input current will double with every 10°C rise in temperature,
and the photodiode’s shunt resistance halves with every 10°C
rise. The error budget in Figure 8 assumes a room temperature
photodiode R
Figure 8. Photodiode Preamp Errors Over Temperature
The capacitance at the amplifier’s negative input (the sum of the
photodiode’s shunt capacitance, the op amp’s differential input
capacitance, stray capacitance due to wiring, etc.) will cause a
rise in the preamp’s noise gain over frequency. This can result in
excess noise over the bandwidth of interest. C
reduces the
F
noise gain “peaking” at the expense of bandwidth.
INSTRUMENTATION AMPLIFIER
The AD548C’s maximum input current of 10 pA makes it an
excellent building block for the high input impedance instrumentation amplifier shown in Figure 9. Total current drain for
this circuit is under 600 µA. This configuration is optimal for
conditioning differential voltages from high impedance sources.
The overall gain of the circuit is controlled by R
, resulting in
G
the following transfer function:
V
OUT
= 1 +
V
IN
(R
+ R2)
1
R
G
Application Hints–AD548
Figure 9. Low Power Instrumentation Amplifier
Gains of 1 to 100 can be accommodated with gain nonlinearities
of less than 0.01%. Input errors, which contribute an output
error proportional to in amp gain, include a maximum untrimmed
input offset voltage of 0.5 mV and an input offset voltage drift
over temperature of 4 µV/°C. Output errors, which are indepen-
dent of gain, will contribute an additional 0.5 mV offset and
4 µV/°C drift. The maximum input current is 15 pA over the
common-mode range, with a common-mode impedance of over
12
1 × 10
matched to 0.01% to take full advantage of the AD548’s high
common-mode rejection. Capacitors C1 and C1′ compensate for
peaking in the gain over frequency caused by input capacitance
when gains of 1 to 3 are used.
The –3 dB small signal bandwidth for this low power instrumentation amplifier is 700 kHz for a gain of 1 and 10 kHz for a gain of
100. The typical output slew rate is 1.8 V/µs.
LOG RATIO AMPLIFIER
Log ratio amplifiers are useful for a variety of signal conditioning
applications, such as linearizing exponential transducer outputs
and compressing analog signals having a wide dynamic range.
The AD548’s picoamp level input current and low input offset
voltage make it a good choice for the front-end amplifier of the
log ratio circuit shown in Figure 10. This circuit produces an
output voltage equal to the log base 10 of the ratio of the input
currents I
voltage inputs.
Input currents I
a matched pair of logging transistors. Voltages at points A and
B are developed according to the following familiar diode
equation:
In this equation, k is Boltzmann’s constant, T is absolute temperature, q is an electron charge, and I
current of the logging transistors. The difference of these two
voltages is taken by the subtractor section and scaled by a factor
of approximately 16 by resistors R9, R10, and R8. Temperature
Ω. Resistor pairs R3/R5 and R4/R6 should be ratio
and I2. Resistive inputs R1 and R2 are provided for
1
and I2 set the collector currents of Q1 and Q2,
1
VBE= (kT/q)ln(IC/IES)
is the reverse saturation
ES
REV. C
–9–
AD548
compensation is provided by resistors R8 and R15 that have a
positive 3500 ppm/°C temperature coefficient. The transfer
function for the output voltage is:
V
= 1V log10(I
OUT
Frequency compensation is provided by R11, R12, C1, and C2.
Small signal bandwidth is approximately 300 kHz at input currents above 100 µA and will proportionally decrease with lower
signal levels. D1, D2, R13, and R14 compensate for the effects
of the two logging transistors’ ohmic emitter resistance.
To trim this circuit, set the two input currents to 10 µA and adjust
V
to zero by adjusting the potentiometer on A3. Then set I
OUT
to 1 µA and adjust the scale factor such that the output voltage is
1 V by trimming potentiometer R10. Offset adjustment for A1 and
A2 is provided to increase the accuracy of the voltage inputs.
This circuit ensures a 1% log conformance error over an input
current range of 300 pA to 1 mA, with low level accuracy
limited by the AD548’s input current. The low level input voltage
accuracy of this circuit is limited by the input offset voltage and
drift of the AD548.