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 a
FEATURES Gain of 20. Alterable from 1 to 160 Input CMR from Below Ground to 6 (VS - 1 V) Output Span 20 mV to (VS - 0.2) V 1-, 2-, 3-Pole Low-Pass Filtering Available Accurate Midscale Offset Capability Differential Input Resistance 400 k Drives 1 k Load to +4 V Using VS = +5 V Supply Voltage: +3.0 V to +36 V Transient Spike Protection and RFI Filters Included Peak Input Voltage (40 ms): 60 V Reversed Supply Protection: -34 V Operating Temperature Range: -40 C to +125 C APPLICATIONS Current Sensing Motor Control Interface for Pressure Transducers, Position Indicators, Strain Gages, and Other Low Level Signal Sources Accelerometers
Single-Supply Sensor Interface Amplifier AD22057
FUNCTIONAL BLOCK DIAGRAM
+VS OFS A1 A2
AD22057
IN+ A1 IN- A2 OUT
GND
GENERAL DESCRIPTION
The AD22057 is a single-supply difference amplifier for amplifying and low-pass filtering small differential voltages (typically 100 mV FS at a gain of 40) from sources having a large commonmode voltage. Supply voltages from +3.0 V to +36 V can be used. The input common-mode range extends from below ground to +24 V using
a +5 V supply with excellent rejection of this common-mode voltage. This is achieved by the use of a special resistive attenuator at the input, laser trimmed to a very high differential balance. Provisions are included for optional low-pass filtering and gain adjustment. An accurate midscale offset feature allows bipolar signals to be amplified.
+VS (CAR BATTERY) SOLENOID LOAD
+5V ANALOG OUTPUT 4V PER AMP
100m
AD22057
200k
CMOS DRIVER C
CORNER FREQUENCY = 0.796Hz- F
CHASSIS
POWER DARLINGTON SINGLE-POLE LOW-PASS FILTERING, GAIN: 40
ANALOG GROUND
Figure 1. Typical Application Circuit for a Current Sensor Interface
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 (c) Analog Devices, Inc., 1999
AD22057-SPECIFICATIONS (T = +25 C, V = +5 V, V
A S
CM
= 0, RL = 10 k
unless otherwise noted)
Min Typ Max +24 -1.0 80 80 180 280 9.7 +0.01 97 90 90 240 0.5 400 10.0 100 2.0 2.0 19.9 -62.5 -1 -12.5 0.49 2.5 7 5 20 20.0 0.03 0.50 3.0 11 30 0.2 0.2 20.1 +62.5 1 +12.5 0.51 25 27 Units V V dB dB k % k V/V V k V/V V V/V ppm/C mV V/C V/V k mA mA kHz V/s V/Hz
Parameter INPUTS (PINS 1 AND 8) +CMR CMR CMRRLF CMRRHF RINCM RMATCH RINDIFF PREAMPLIFIER GCL VO RO OUTPUT BUFFER GCL VO RO OVERALL SYSTEM G VOS OFS IOSC BW-3 dB SR NSD PSR
Comments Positive Common-Mode Range Negative Common-Mode Range Common-Mode Rejection Ratio Common-Mode Rejection Ratio Common-Mode Input Resistance Matching of Resistances Differential Input Resistance Closed-Loop Gain1 Output Voltage Range (Pin 3) Output Resistance2 Closed-Loop Gain1 Output Voltage Range3 Output Resistance (Pin 5) Gain1 Gain Drift Input Offset Voltage4 Offset Drift Midscale Offset (Pin 7) Scaling Input Resistance Short-Circuit Output Current -3 dB Bandwidth Slew Rate Noise Spectral Density4 Power Supply Rejection Input Offset Voltage4 Gain Operating Range Quiescent Supply Range5 Operating Temperature Range Plastic Mini-DIP (N-8) Plastic SOIC (SO-8)
Test Conditions TA = TMIN to TMAX TA = TMIN to +85C f 10 Hz f = 1 kHz Pin 1 or Pin 8 to Pin 2 Pin 1 to Pin 8
300
10.3 +4.8 103 2.06 +4.8
RLOAD 10 k VO 0.1 V dc VO 0.1 V dc TA = TMIN to TMAX TA = TMIN to TMAX Pin 7 to Pin 2 TA = TMIN to TMAX VO = +1 V dc f = 100 Hz to 10 kHz VS = 5 V, VO = 1 V to 4.2 V VS = 24 V, VO = 1 V to 22 V TA = TMIN to TMAX
1.94 +0.02
VOS G POWER SUPPLY VS IS TEMPERATURE RANGE TOP PACKAGE
20.0 0.05 TA = TMIN to TMAX TA = +25C, VS = +5 V 3 5 200 36 500 +125 AD22057N AD22057R
V/V %/V V A C
-40
NOTES 1 Specified for default mode i.e., with no external components. The overall gain is trimmed to 0.5% while the individual gains of A1 and A2 may be subject to a maximum 3% tolerance. Note that the actual gain in a particular application can be modified by the use of external resistor networks. 2 The actual output resistance of A1 is only a few ohms, but access to this output, via Pin 3, is always through a 100 k resistor, which is trimmed to 3%. 3 For VCM 20 V. For V CM > 20 V, VOL 1 mV/V x VCM. 4 Referred to the input (Pins 1 and 8). 5 With VDM = 0 V. Differential mode signals are referred to as V DM, while VCM refers to common-mode voltages. Specifications subject to change without notice.
ORDERING GUIDE
Model AD22057N AD22057R AD22057R-Reel
Temperature Range -40C to +125C -40C to +125C -40C to +125C
Package Descriptions Plastic DIP Plastic SOIC Tape and Reel
Package Options N-8 SO-8 SO-8*
*Quantities must be in increments of 2,500 pieces each.
-2-
REV. A
AD22057
ABSOLUTE MAXIMUM RATINGS* PIN CONFIGURATIONS Plastic Mini-DIP Package (N-8)
-IN 1 GND 2
8
Supply Voltage . . . . . . . . . . . . . . . . . . . . . . . . +3.0 V to +36 V Peak Input Voltage (40 ms) . . . . . . . . . . . . . . . . . . . . . . +60 V VOFS (Pin 7 to Pin 2) . . . . . . . . . . . . . . . . . . . . . . . . . . . . +20 V Reversed Supply Voltage Protection . . . . . . . . . . . . . . . -34 V Operating Temperature . . . . . . . . . . . . . . . . -40C to +125C Storage Temperature . . . . . . . . . . . . . . . . . . -65C to +150C Output Short Circuit Duration . . . . . . . . . . . . . . . . Indefinite Lead Temperature Range (Soldering 60 sec) . . . . . . . . +300C
*Stresses above those listed under Absolute Maximum Ratings may cause permanent damage to the device. This is a stress rating only; the 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.
Plastic SOIC Package (SO-8)
-IN 1 GND 2
8
+IN OFFSET
+IN
AD22057
7
TOP VIEW A1 3 (Not to Scale) 6 +VS A2 4
5
OFFSET TOP VIEW A1 3 (Not to Scale) 6 +VS
7
AD22057
OUT
A2 4
5
OUT
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 AD22057 features proprietary ESD protection circuitry, permanent damage may occur on devices subjected to high energy electrostatic discharges. Therefore, proper ESD precautions are recommended to avoid performance degradation or loss of functionality.
WARNING!
ESD SENSITIVE DEVICE
PRODUCT DESCRIPTION
The AD22057 is a single-supply difference amplifier consisting of a precision balanced attenuator, a very low drift preamplifier and an output buffer amplifier (A1 and A2, respectively, in Figure 2). It has been designed so that small differential signals (VDM in Figure 3) can be accurately amplified and filtered in the presence of large common-mode voltages (VCM) without the use of any other active components.
+VS OFS A1 A2
offset to an optional voltage of one half of that supplied to Pin 7; in many cases this offset would be +VS/2 by tying Pin 7 to +VS (Pin 6), permitting the conditioning and processing of bipolar signals (see Strain Gage Interface section). The output buffer A2 has a gain of x2, setting the precalibrated, overall gain of the AD22057, with no external components, to x20. (This gain is easily user-configurable--see Altering the Gain section for details.) The dynamic properties of the AD22057 are optimized for interfacing to transducers; in particular, current sensing shunt resistors. Its rejection of large, high frequency, common-mode signals makes it superior to that of many alternative approaches. This is due to the very careful design of the input attenuator and the close integration of this highly balanced, high impedance system with the preamplifier.
APPLICATIONS
AD22057
IN+ A1 IN- A2 OUT
GND
Figure 2. Simplified Schematic
The resistive attenuator network is situated at the input to the AD22057 (Pins 1 and 8), allowing the common-mode voltage at Pins 1 and 8 to be six times greater than that which can be tolerated by the actual input to A1. As a result, the input commonmode range extends to 6x (VS - 1 V). Two small filter capacitors (not shown in Figure 2) have been included at the inputs of A1 to minimize the effects of any spurious RF signals present in the signal. Internal feedback around A1 sets the closed-loop gain of the preamplifier to x10 from the input pins; the output of A1 is connected to Pin 3 via a 100 k resistor, which is trimmed to 3% (R12 in Figure 2) to facilitate the low-pass filtering of the signal of interest (see Low-Pass Filtering section). The inclusion of an additional resistive network allows the output of A1 to be
The AD22057 can be used wherever a high gain, single-supply differencing amplifier is required, and where a finite input resistance (240 k to ground, 400 k between differential inputs) can be tolerated. In particular, the ability to handle a commonmode input considerably larger than the supply voltage is frequently of value. Also, the output can run down to within 20 mV of ground, provided it is not called on to sink any load current. Finally, the output can be offset to half of a full-scale reference voltage (with a tolerance of 2%) to allow a bipolar input signal.
ALTERING THE GAIN
The gain of the preamplifier, from the attenuator input (Pins 1 and 8) to its output at Pin 3, is x10 and that of the output buffer, from Pin 4 to Pin 5, is x2, thus making the overall default gain x20. The overall gain is accurately trimmed (to within 0.5%). In some cases, it may be desirable to provide for some variation in the gain; for example, in absorbing the scaling error of a transducer.
REV. A
-3-
AD22057
Figure 3 shows a general method for trimming the gain, either upward or downward, by an amount dependent on the resistor, R. The gain range, expressed as a percentage of the overall gain, is given by (10 M/R)%. Thus, the adjustment range would be 2% for R = 5 M; 10% for R = 1 M, etc.
ANALOG OUTPUT +IN VDM OFS +VS OUT
AD22057
-IN GND A1 A2 R GAIN ADJUST 20k MIN ANALOG COMMON
Increasing the Gain. The gain can be raised by connecting a resistor from the output of the buffer amplifier (Pin 5) to its noninverting input (Pin 4) as shown in Figure 5. The gain is now multiplied by the factor R/(R-100k); for example, it is doubled for R = 200 k. Overall gains of up to x160 (R = 114 k) are readily achievable in this way. Note, however, that the accuracy of the gain becomes critically dependent on resistor value at high gains. Also, the effective input offset voltage at Pins 1 and 8 (about six times the actual offset of A1) limits the part's use in very high gain, dc-coupled applications. The gain may be trimmed by using a fixed and variable resistor in series (see, for example, Figure 10).
ANALOG OUTPUT +IN OFS +VS OUT VDM
VCM
(SEE TEXT)
VDM = DIFFERENTIAL VOLTAGE, VCM = COMMOM-MODE VOLTAGE
Figure 3. Altering Gain to Accommodate Transducer Scaling Error
AD22057
-IN GND A1 A2 POINT X (SEE TEXT)
20R GAIN = --------- R - 100k R GAIN R = 100k --------- GAIN - 20 ANALOG COMMON
In addition to the method above, another method may be used to vary the gain. Many applications will call for a gain higher than x20, and some require a lower gain. Both of these situations are readily accommodated by the addition of one external resistor, plus an optional potentiometer if gain adjustment is required (for example, to absorb a calibration error in a transducer). Decreasing the Gain. See Figure 4. Since the output of the preamplifier has an output resistance of 100 k, an external resistor connected from Pin 4 to ground will precisely lower the gain by a factor R/(100k+R). When configuring the AD22057 for any gain, the maximum input and the power supply being used should be considered, since either the preamplifier or the output buffer will reach its full-scale output (approximately VS - 0.2 V) with large differential input voltages. The input of the AD22057 is limited to no greater than (V - 0.2)/10, for overall gains less than 10, since the preamplifier, with its fixed gain of x10, reaches its full scale output before the output buffer. For VS = 5 V this is 0.48 V. For gains greater than 10, however, the swing at the buffer output reaches its full-scale first and limits the AD22057 input to (VS - 0.2)/G, where G is the overall gain. Increasing the power supply voltage increases the allowable maximum input. For VS = 5 V and a nominal gain of 20, the maximum input is 240 mV. The overall bandwidth is unaffected by changes in gain using this method, although there may be a small offset voltage due to the imbalance in source resistances at the input to A2. In many cases this can be ignored but, if desired, can be nulled by inserting a resistor in series with Pin 4 (at "Point X" in Figure 4) of value 100 k minus the parallel sum of R and 100 k. For example, with R = 100 k (giving a total gain of x10), the optional offset nulling resistor is 50 k.
ANALOG OUTPUT +IN VDM OFS +VS OUT
VCM
Figure 5. Achieving Gains Greater Than x20
Once again, a small offset voltage will arise from an imbalance in source resistances and the finite bias currents inherently present at the input of A2. In most applications this additional offset error (about 130 V at x40) will be comparable with the specified offset range and will therefore introduce negligible skew. It may, however, be essentially eliminated by the addition of a resistor in series with the parallel sum of R and 100 k (i.e., at "Point X" in Figure 5) so the total series resistance is maintained at 100 k. For example, at a gain of x30, when R = 300 k and the parallel sum of R and 100 k is 75 k, the padding resistor should be 25 k. A 50 k pot would provide an offset range of about 2.25 mV referred to the output, or 75 V referred to the attenuator input. A specific example is shown in Figure 12.
LOW-PASS FILTERING
In many transducer applications it is necessary to filter the signal to remove spurious high frequency components, including noise, or to extract the mean value of a fluctuating signal with a peak-to-average ratio (PAR) greater than unity. For example, a full wave rectified sinusoid has a PAR of 1.57, a raised cosine has a PAR of 2 and a half wave sinusoid has a PAR of 3.14. Signals having large spikes may have PARs of 10 or more. When implementing a filter, the PAR should be considered so the output of the AD22057 preamplifier (A1) does not clip before A2 does, since this nonlinearity would be averaged and appear as an error at the output. To avoid this error both amplifiers should be made to clip at the same time. This condition is achieved when the PAR is no greater than the gain of the second amplifier (2 for the default configuration). For example, if a PAR of 5 is expected, the gain of A2 should be increased to 5. Low-pass filters can be implemented in several ways using the features provided by the AD22057. In the simplest case, a single-pole filter (20 dB/decade) is formed when the output of A1 is connected to the input of A2 via the internal 100 k resistor by strapping Pins 3 and 4, and a capacitor added from this node to ground, as shown in Figure 6. The dc gain remains x20, and the gain trim shown in Figure 3 may still be used. If a resistor is added across the capacitor to lower the gain, the corner -4- REV. A
AD22057
-IN GND A1 A2
20R GAIN = --------- R + 100k GAIN R = 100k --------- 20 - GAIN
VCM
R
POINT X (SEE TEXT) ANALOG COMMON
Figure 4. Achieving Gains Less Than x20
AD22057
frequency will increase; it should be calculated using the parallel sum of the resistor and 100 k.
ANALOG OUTPUT 1 100k
+IN OFS +VS OUT VDM
CORNER FREQUENCY = THAT IS, 1.59Hz- F
AD22057
-IN GND A1 A2
2C
A three-pole filter (with roll-off 60 dB/decade) can be formed by adding a passive RC network at the output forming a real pole. A three-pole filter with a corner frequency f3 has the same attenuation a one-pole filter of corner f1 has at a frequency f33/f1, where the attenuation is 30 Log (f3/f1) (see the graph in Figure 9). Using equal capacitor values, and a resistor of 160 k, the corner-frequency calibration remains 1 Hz-F.
FREQUENCY ATTENUATION
(C IS IN FARADS) VCM C ANALOG COMMON
-20dB/DECADE
-60dB/DECADE
Figure 6. Connections for Single-Pole, Low-Pass Filter
If the gain is raised using a resistor, as shown in Figure 5, the corner frequency is lowered by the same factor as the gain is raised. Thus, using a resistor of 200 k (for which the gain would be doubled) the corner frequency is now 0.796 Hz-F, (0.039 F for a 20 Hz corner).
ANALOG OUTPUT +IN OFS +VS OUT VDM
30LOG (f3/f1)
A 1-POLE FILTER, CORNER f1, AND A 3-POLE FILTER, CORNER f3, HAVE THE SAME ATTENUATION, -30LOG (f3/f1), AT FREQUENCY (f33/f1)
f1
f3
(f33/f1)
AD22057
-IN GND A1 A2 255k
C CORNER FREQUENCY = 1Hz- F
Figure 9. Comparative Responses of One- and Three-Pole Low-Pass Filters
CURRENT SENSOR INTERFACE
VCM
C
ANALOG COMMON
A typical automotive application making use of the large common-mode range is shown in Figure 10.
+VS (BATTERY) SOLENOID LOAD FLYBACK DIODE +IN OFS +VS OUT 100m 191k 5% SENSOR CALIBRATION 20k CORNER FREQUENCY = 0.796Hz- F (0.22 F FOR f = 3.6Hz) ANALOG COMMON +5V
Figure 7. Connections for Conveniently Scaled, Two-Pole, Low-Pass Filter
A two-pole filter (with a roll-off of 40 dB/decade) can be implemented using the connections shown in Figure 7. This is a Sallen & Key form based on a x2 amplifier. It is useful to remember that a two-pole filter with a corner frequency f2 and a one-pole filter with a corner at f1 have the same attenuation at the frequency (f22/f1). The attenuation at that frequency is 40 Log(f2/f1). This is illustrated in Figure 8. Using the standard resistor value shown, and equal capacitors (in Figure 7), the corner frequency is conveniently scaled at 1 Hz-F (0.05 F for a 20 Hz corner). A maximally flat response occurs when the resistor is lowered to 196 k and the scaling is then 1.145 HzF. The output offset is raised by about 4 mV (equivalent to 200 V at the input pins).
FREQUENCY ATTENUATION -40dB/DECADE
ANALOG OUTPUT 4V PER AMP
AD22057
-IN GND A1 A2
CMOS DRIVER C POWER DARLINGTON
CHASSIS
Figure 10. Current Sensor Interface. Gain Is x40, SinglePole Low-Pass Filtering
-20dB/DECADE
40LOG (f2/f1)
A 1-POLE FILTER, CORNER f1, AND A 2-POLE FILTER, CORNER f2, HAVE THE SAME ATTENUATION, -40LOG (f2/f1), AT FREQUENCY f22/f1
The current in a load, here shown as a solenoid, is controlled by a power transistor that is either cut off or saturated by a pulse at its base; the duty-cycle of the pulse determines the average current. This current is sensed in a small resistor. The average differential voltage across this resistor is typically 100 mV, although its peak value will be higher by an amount that depends on the inductance of the load and the control frequency. The common-mode voltage, on the other hand, extends from roughly 1 V above ground, when the transistor is saturated, to about 1.5 V above the battery voltage, when the transistor is cut off and the diode conducts. If the maximum battery voltage spikes up to +20 V, the commonmode voltage at the input can be as high as 21.5 V. This can be measured using even a +5 V supply for the AD22057.
f1
f2
(f22/f1)
Figure 8. Comparative Responses of One- and Two-Pole Low-Pass Filters
REV. A
-5-
AD22057
To produce a full-scale output of +4 V, a gain x40 is used, adjustable by 5% to absorb the tolerance in the sense resistor. There is sufficient headroom to allow at least a 10% overrange (to +4.4 V). The roughly triangular voltage across the sense resistor is averaged by a single-pole low-pass filter, here set with a corner frequency of fC = 3.6 Hz, which provides about 30 dB of attenuation at 100 Hz. A higher rate of attenuation can be obtained by a two-pole filter having fC = 20 Hz, as shown in Figure 11. Although this circuit uses two separate capacitors, the total capacitance is less than half that needed for the single-pole filter.
+5V +VS (BATTERY) SOLENOID LOAD 432k +IN 100m OFS +VS OUT C 50k A2 127k CMOS DRIVER C CHASSIS POWER DARLINGTON CORNER FREQUENCY = 1Hz- F (0.05 F FOR fC= 20Hz) ANALOG COMMON
A2 OUT
An ac excitation of up to 2 V can also be used because the common-mode range of the AD22057 extends to -1 V. Assuming a full-scale bridge output (VG) of 10 mV, a gain of x100 might be used to provide an output of 1 V (a full-scale range of +1.5 V to +3.5 V). This gain is achieved using the method discussed in connection with Figure 5. Note that the gainsetting resistor does not affect the accuracy of the midscale offset. (However, if the gain were lowered, using a resistor to ground, this offset would no longer be accurate.) A VOS nulling pot is included for illustrative purposes. One-, two- and threepole filtering can also be implemented, as discussed in the Low-Pass Filtering section.
Using the Midscale Offset Feature
ANALOG OUTPUT
FLYBACK DIODE
AD22057
-IN GND A1
Figure 13 shows a more detailed schematic of the output amplifier A2. Because this is a single supply device, the output stage has no pull-down transistor. Such a transistor would limit the minimum output to several hundred millivolts above ground. When using the AD22057 in unipolar mode (Pin 7 grounded), the resistors making up the feedback network also act as a pull-down for the output stage.
+VS
Figure 11. Illustration of Two-Pole Low-Pass Filtering
95k
10k RL 20k OFS 20k GND
STRAIN GAGE INTERFACE: MIDSCALE OFFSET FEATURE
The AD22057 can be used to interface a strain gage to a subsequent process where only a single supply voltage is available. In this application, the midscale offset feature is valuable, since the output of the bridge may have either polarity. Figure 12 shows typical connections.
+VS ANALOG OUTPUT R VG R R R +IN OFS +VS OUT 125k (SETS GAIN TO 100) RL 10k
Figure 13. Detailed Schematic of Output Amplifier A2
AD22057
-IN GND A1 A2
100k VOS NULL OPTIONAL LP FILTER
If the output is called upon to source current (not sink), then it can swing almost completely to ground (within 20 mV). However, if the offset pin is connected to some positive voltage source, this source will "pull up" the output voltage, thereby limiting the minimum output swing. With no external load the minimum output voltage possible is VOFS/2. For example, if Pin 7 is connected to +5 V, the minimum output voltage is equal to the offset voltage of 2.5 V. By adding an additional load, as shown, the output swing toward ground can be extended. The relationship is described by:
ANALOG COMMON
Figure 12. Typical Connections for a Strain Gage Interface Using the Offset Feature
1 RL VOUT > VOFS RL + 20 k * 2
*This 20 k resistor is internal to the AD22057 and can vary by 30%.
The offset is obtained by connecting Pin 7 (OFS) to the supply voltage. In this way, the output of the AD22057 is centered to midway between the supply and ground. In many systems the supply will also serve as the reference voltage for a subsequent A/D converter. Alternatively, Pin 7 may be tied to the reference voltage from an independent source. The AD22057 is trimmed to guarantee an accuracy of 2% on the 0.5 ratio between the voltage on Pin 7 and the output.
where RL is an externally applied load resistor. However, RL cannot be made arbitrarily small since this would require excessive current from the output. The output current should be limited to 5 mA total.
-6-
REV. A
AD22057
APPLICATION HINTS Frequency Compensation
As are all closed-loop op amp circuits, the AD22057 is sensitive to capacitive loading at its output. However, the AD22057 is sensitive at higher output voltages due to nonlinear effects in the rail-to-rail design of the buffer amplifier (A2). In this amplifier the output stage gain increases with increasing output voltage. This behavior does not affect dc parameters such as gain accuracy or linearity; however, it can compromise ac stability. When operating from a power supply of 5 V or less (and, therefore, VOUT < 5 V), the AD22057 can drive capacitive loads up to 25 pF with no external components. When operating at higher supply voltages (which are associated with higher output voltages) and/or driving larger capacitive loads, an external compensation network should be used. Figure 14 shows an R-C "snubber" circuit loading the output of the AD22057. This combination, in conjunction with the internal 20 k resistance, forms a lag network. This network attenuates the openloop gain of the amplifier at higher frequencies. The ratio of RLAG to the load seen by the AD22057 determines the high frequency attenuation seen by the op amp. If RLAG is made 1/20th of the total load resistance (20 k RL), then 26 dB of attenuation is obtained at higher frequencies. The capacitor (CLAG) is used to control the frequency of the compensation network. It should be set to form a 5 s time constant with the resistor (RLAG). Table I shows the recommended values of RLAG and CLAG for various values of external load resistor RL. Ten percent tolerance on these components is acceptable. Alternatively, the signal may be taken from the midpoint of RLAG-CLAG. This output is particularly useful when driving CMOS analog-to-digital converters. For more information see the section Driving Charged Redistributed A/D Converters. Note that when implementing this network large signal response is compromised. This occurs because there is no active pull-down and the lag capacitor must discharge through the internal feedback resistor (20 k) giving a fairly long-time constant. For example if CLAG = 0.01 F, the large signal negative slew characteristic is a decaying exponential with a time constant of 200 s.
Table I. Compensation Components vs. External Load Resistor
network helps to absorb the additional charge, effectively lowering the high frequency output impedance of the AD22057. For these applications the output signal should be taken from the midpoint of the RLAG-CLAG combination as shown in Figure 15. Since the perturbations from the analog-to-digital converter are small, the output of the AD22057 will appear to be a low impedance. The transient response will, therefore, have a time constant governed by the product of the two lag components, CLAG x RLAG. For the values shown in Figure 15, this time constant is programmed at approximately 10 s. Therefore, if samples are taken at several tens of microseconds or more, there will be negligible "stacking up" of the charge injections.
+VS
AD22057
A2
10k RLAG CLAG 10k LOAD
RL
CL
Figure 14. Using an R-C Network for Compensation
+VS
AD22057
A2
10k 1k IN 0.01 F PROCESSOR A/D
10k
Figure 15. Recommended Circuit for Driving CMOS A/D Converters
UNDERSTANDING THE AD22057
RL >100 k > 50 k > 20 k > 10 k > 5 k > 2 k
RLAG 470 390 270 200 100 47
CLAG 0.01 F 0.01 F 0.047 F 0.047 F 0.1 F 0.22 F
Figure 16 shows the main elements of the AD22057. The signal inputs at Pins 1 and 8 are first applied to dual resistive attenuators R1 through R4, whose purpose is to reduce the commonmode voltage at the input to the preamplifier. The attenuated signal is then applied to a feedback amplifier based on the very low drift op amp, A1. The differential voltage across the inputs is accurately amplified in the presence of common-mode voltages of many times the supply voltage. The overall commonmode response is minimized by precise laser trimming of R3 and R4, giving the AD22057 a common-mode rejection ratio (CMRR) of at least 80 dB (10,000:1). The common-mode range of A1 extends from slightly below ground to 1 V below +VS (at the minimum temperature of -40C). Since an attenuation ratio of about 6 is used, the input common-mode range is -1 V to +24 V using a +5 V supply. Small filter capacitors C1 and C2 are included to minimize the effects of spurious RF signals at the inputs, which might cause dc errors due to the rectification effects at the input to A1. At high frequencies, even a small imbalance in these components would seriously degrade the CMRR, so a special high frequency trim is also carried out during manufacture.
Driving Charge Redistribution A/D Converters
When driving CMOS ADCs, such as those embedded in popular microcontrollers, the charge injection (Q) can cause a significant deflection in the AD22057 output voltage. Though generally of short duration, this deflection may persist until after the sample period of the ADC has expired. It is due to the relatively high open-loop output impedance of the AD22057. The effect can be significantly reduced by including the same R-C network recommended for improving stability (see Frequency Compensation section). The large capacitor in the lag REV. A
-7-
AD22057
A unique method of feedback around A1, provided by R9 and R7, sets the closed-loop gain of the preamplifier to x10 (from the input pins). The feedback network is balanced by the inclusion of R6 and R8. The small value of R7 results in a more practical value for R9 (which would have to be 2 M if the feedback were taken directly to the inputs of A1). R8 is not directly connected to ground, but to an optional voltage of one half that is applied to Pin 7 (OFS). It is trimmed to within close tolerances through R10 and R11. This allows the output of A1 to be offset to midscale, typically +VS/2, by tying Pins 6 and 7 together. (For an example of the use of this feature, see Figure 12.) The gain is adjusted by the single resistor R5, which acts only on the differential signal. More importantly, it also results in much less feed forward of the common-mode signal to the output of A1, which, being a single-supply circuit, has no means of pulling this output down toward ground in those circumstances where the common-mode input is very positive while the net differential signal is small. (The output of A1 is the collector of a PNP transistor whose emitter is tied to +VS.) R16 is specifically included to alleviate this problem. The output of the preamplifier is connected to Pin 3 via R12, a 100 k resistor that is trimmed to within 3%. The inclusion of R12 allows a low-pass filter to be formed, with an accurate time constant, by placing a capacitor from Pin 3 to ground. By separating the connections at Pins 3 and 4, a two-pole Sallen and Key filter can be formed (see Low-Pass Filtering section) and also provides a means for setting the overall gain to values other than x20 (see Altering the Gain section). The output buffer has a gain of x2, set by the feedback network around op amp A2, formed by R15 and R13 R14. Note that this gain is not trimmed to a precise value, but may have a tolerance of 3% (max). Only the overall gain of A1 and A2 is trimmed to within 0.5% by R5. As a consequence, the gain of A1 may be in error by 3% (max) as the trim to R5 absorbs the initial error in the gain of A2. In most applications Pins 3 and 4 are simply tied together, but the output buffer can be used independently if desired. The offset voltage of A2 is nulled during manufacture. R17 is included to minimize the offset due to bias currents. It is recommended, in applications where A2 is used independently and the source resistance is less than 100 k, that the necessary extra resistance should be included. The output of A2 is the collector of a PNP transistor whose emitter is tied to +VS. The bias current out of the inverting input of this amplifier generates an offset voltage of about +1 mV in R13 R14, which is passed directly to the output via R15. This sets the lowest output that can be reached when there is no load resistor. However, the output can drive a 1 k load to at least +4.5 V when +VS = +5 V. If operation to much lower minimum voltages is essential, a load resistor can be added externally.
+VS R1 200k IN+ IN- R2 200k R8 9k R11 2k R10 2k R3 41k R5 2.6k R6 250k R4 41k R7 250 A1 R12 100k A1 C2 5pF R9 10k R16 10k R13 20k OFS R17 95k A2 R15 10k R14 20k GND OUT A2
AD22057
R18 1k R19 1k
C1 5pF
Figure 16. Simplified Schematic of AD22057, Including Component Values
OUTLINE DIMENSIONS
Dimensions shown in inches and (mm).
Plastic Mini-DIP Package (N-8)
0.430 (10.92) 0.348 (8.84)
8 5
Plastic SOIC Package (SO-8)
0.1968 (5.00) 0.1890 (4.80)
0.280 (7.11) 0.240 (6.10)
1 4
PIN 1 0.210 (5.33) MAX
0.060 (1.52) 0.015 (0.38) 0.130 (3.30) MIN SEATING PLANE
0.325 (8.25) 0.300 (7.62) 0.195 (4.95) 0.115 (2.93)
0.1574 (4.00) 0.1497 (3.80)
8 1
5 4
0.2440 (6.20) 0.2284 (5.80)
0.160 (4.06) 0.115 (2.93) 0.022 (0.558) 0.100 0.070 (1.77) 0.014 (0.356) (2.54) 0.045 (1.15) BSC
PIN 1 0.0098 (0.25) 0.0040 (0.10)
0.0688 (1.75) 0.0532 (1.35)
0.0196 (0.50) 0.0099 (0.25)
45
0.015 (0.381) 0.008 (0.204)
0.0500 0.0192 (0.49) SEATING (1.27) 0.0098 (0.25) PLANE BSC 0.0138 (0.35) 0.0075 (0.19)
8 0
0.0500 (1.27) 0.0160 (0.41)
-8-
REV. A
PRINTED IN U.S.A.
C2181a-2-4/99


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