Data Sheet AD823
Rev. E | Page 15 of 20
APPLICATION NOTES
INPUT CHARACTERISTICS
In the AD823, N-Channel JFETs are used to provide a low offset,
low noise, high impedance input stage. Minimum input common-
mode voltage extends from 0.2 V below −V
S
to 1 V < +V
S
. Driving
the input voltage closer to the positive rail causes a loss of amplifier
bandwidth and increased common-mode voltage error.
The AD823 does not exhibit phase reversal for input voltages up
to and including +V
S
. Figure 38 shows the response of an AD823
voltage follower to a 0 V to 5 V (+V
S
) square wave input. The
input and output are superimposed. The output polarity tracks
the input polarity up to +V
S
, with no phase reversal. The reduced
bandwidth above a 4 V input causes the rounding of the output
wave form. For input voltages greater than +V
S
, a resistor in
series with the AD823’s noninverting input prevents phase
reversal, at the expense of greater input voltage noise. This is
illustrated in Figure 39.
GND
100
0%
1V
2µs
1V
90
00901-038
10
Figure 38. AD823 Input Response: R
P
= 0, V
IN
= 0 to +V
S
+V
S
GND
5V
V
IN
R
P
V
OUT
AD823
1V
10µs1V
00901-039
90
100
10
0%
Figure 39. AD823 Input Response:
V
IN
= 0 to +V
S
+ 200 mV, V
OUT
= 0 to +V
S
, R
P
= 49.9 kΩ
Because the input stage uses N-Channel JFETs, input current
during normal operation is negative; the current flows out from
the input terminals. If the input voltage is driven more positive
than +V
S
− 0.4 V, the input current reverses direction as internal
device junctions become forward biased. This is illustrated in
Figure 7.
A current limiting resistor should be used in series with the
input of the AD823 if there is a possibility of the input voltage
exceeding the positive supply by more than 300 mV, or if an
input voltage is applied to the AD823 when ±V
S
= 0. The
amplifier becomes damaged if left in that condition for more
than 10 seconds. A 1 kΩ resistor allows the amplifier to
withstand up to 10 V of continuous overvoltage and increases
the input voltage noise by a negligible amount.
Input voltages less than −V
S
are a completely different story.
The amplifier can safely withstand input voltages 20 V below
−V
S
as long as the total voltage from the positive supply to the
input terminal is less than 36 V. In addition, the input stage
typically maintains picoamp level input currents across that
input voltage range.
The AD823 is designed for 16 nV/√Hz wideband input voltage
noise and maintains low noise performance to low frequencies
(see Figure 16). This noise performance, along with the AD823’s
low input current and current noise, means that the AD823
contributes negligible noise for applications with source
resistances greater than 10 kΩ and signal bandwidths greater
than 1 kHz.
OUTPUT CHARACTERISTICS
The AD823’s unique bipolar rail-to-rail output stage swings
within 25 mV of the supplies with no external resistive load.
The AD823’s approximate output saturation resistance is 25 Ω
sourcing and sinking. This can be used to estimate the output
saturation voltage when driving heavier current loads. For
instance, when driving 5 mA, the saturation voltage to the rails
is approximately 125 mV.
If the AD823’s output is driven hard against the output
saturation voltage, it recovers within 250 ns of the input
returning to the amplifier’s linear operating region.
A/D Driver
The rail-to-rail output of the AD823 makes it useful as an A/D
driver in a single-supply system. Because it is a dual op amp, it
can be used to drive both the analog input of the A/D as well as
its reference input. The high impedance FET input of the
AD823 is well suited for minimal loading of high output
impedance devices.
AD823 Data Sheet
Rev. E | Page 16 of 20
Figure 40 shows a schematic of an AD823 being used to drive
both the input and reference input of an AD1672, a 12-bit,
3-MSPS, single-supply ADC. One amplifier is configured as a
unity-gain follower to drive the analog input of the AD1672,
which is configured to accept an input voltage that ranges from
0 V to 2.5 V.
The other amplifier is configured as a gain of 2 to drive the
reference input from a 1.25 V reference. Although the AD1672
has its own internal reference, there are systems that require
greater accuracy than the internal reference provides. On the other
hand, if the AD1672 internal reference is used, the second AD823
amplifier can be used to buffer the reference voltage for driving
other circuitry while minimally loading the reference source.
13
14
12
11
10
9
8
7
6
5
4
3
2
1
19 18
+5VA
10µF
0.1µF
2
3
5
6
4
7
1
8
49.9
10µF
0.1µF
0.1µF 10µF
0.1µF
+5
V
A
+5VD
+5VD
20
21
22
23
24
25
26
27
16
CLOCK
1k
1k
V
IN
V
REF
(1.25V)
BIT1 (MSB)
BIT2
BIT3
BIT4
BIT5
BIT6
BIT7
BIT8
BIT9
BIT10
BIT11
BIT12 (LSB)
15
OTR
REFOUT
AIN1
AIN2
REFIN
REFCOM
NCOMP2
NCOMP1
ACOM
COM
REF
DCOM
AD823
+V
CC
+V
DD
28 19
AD1672
00901-040
Figure 40. AD823 Driving Input and Reference of the
AD1672, a 12-Bit, 3-MSPS ADC
The circuit was tested with a 500 kHz sine wave input that was
heavily low-pass filtered (60 dB) to minimize the harmonic content
at the input to the AD823. The digital output of the AD1672 was
analyzed by performing a fast Fourier transform (FFT).
During the testing, it was observed that at 500 kHz, the output
of the AD823 cannot go below ~350 mV (operating with
negative supply at ground) without seriously degrading the
second harmonic distortion. Another test was performed with a
200 Ω pull-down resistor to ground that allowed the output to
go as low as 200 mV without seriously affecting the second
harmonic distortion. There was, however, a slight increase in
the third harmonic term with the resistor added, but it was still
less than the second harmonic.
Figure 41 is an FFT plot of the results of driving the AD1672
with the AD823 with no pull-down resistor. The input
amplitude was 2.15 V p-p and the lower voltage excursion was
350 mV. The input frequency was 490 kHz, which was chosen
to spread the location of the harmonics.
The distortion analysis is important for systems requiring good
frequency domain performance. Other systems may require
good time domain performance. The noise and settling time
performance of the AD823 provides the necessary information
for its applicability for these systems.
5
6
9
3
1
V
IN
= 2.15V p-p
G = +1
FI = 490kHz
15dB/DI
V
7
8
00901-041
2
4
Figure 41. FFT of AD1672 Output Driven by AD823
3 V, Single-Supply Stereo Headphone Driver
The AD823 exhibits good current drive and total harmonic
distortion plus noise (THD+N) performance, even at 3 V
single supplies. At 20 kHz, THD+N equals −62 dB (0.079%) for
a 300 mV p-p output signal. This is comparable to other single-
supply op amps that consume more power and cannot run on
3 V power supplies.
In Figure 42, each channels input signal is coupled via a 1 μF
Mylar capacitor. Resistor dividers set the dc voltage at the
noninverting inputs so that the output voltage is midway
between the power supplies (+1.5 V). The gain is 1.5. Each half
of the AD823 can then be used to drive a headphone channel. A
5 Hz high-pass filter is realized by the 500 μF capacitors and the
headphones that can be modeled as 32 Ω load resistors to
ground. This ensures that all signals in the audio frequency
range (20 Hz to 20 kHz) are delivered to the headphones.
MYLAR
1µF
1/2
AD823
L
R
HEADPHONES
32 IMPEDANCE
4.99k
MYLAR
1µF
4.99k
10k
10k
47.5k
95.3k
47.5k
500µF
500µF
3V
95.3k
0.1µF
+
0.1µF
CHANNEL 1
CHANNEL 2
95.3k
+
+
7
4
5
6
1/2
AD823
3
8
2
1
1
00901-042
Figure 42. 3 V Single-Supply Stereo Headphone Driver
Data Sheet AD823
Rev. E | Page 17 of 20
Second-Order Low-Pass Filter
Figure 43 depicts the AD823 configured as a second-order
Butterworth low-pass filter. With the values as shown, the
corner frequency equals 200 kHz. Component selection is
shown in the following equations:
R1 = R2 = User Selected (Typical Values: 10 kΩ to 100 kΩ)

R1f
.
faradsC1
cutoff
4141
R1f
C2
cutoff
707.0
1/2
AD823
C3
0.1µF
+5V
C4
0.1µF
V
OUT
V
IN
C1
28pF
–5V
C2
56pF
R1
20k
R2
20k
50pF
00901-043
Figure 43. Second-Order Low-Pass Filter
A plot of the filter is shown in Figure 44; better than 50 dB of
high frequency rejection is provided.
FREQUENCY (Hz)
–40
HIGH FREQUENCY REJECTION (dB)
1k
–50
–30
–60
0
–20
10k 100k
1M
10M 100M
–10
V
DB
– V
OUT
00901-044
Figure 44. Frequency Response of Filter
Single-Supply Half-Wave and Full-Wave Rectifiers
An AD823 configured as a unity-gain follower and operated
with a single supply can be used as a simple half-wave rectifier.
The AD823 inputs maintain picoamp level input currents even
when driven well below the minus supply. The rectifier puts
that behavior to good use, maintaining an input impedance of
over 10
11
Ω for input voltages from within 1 V of the positive
supply to 20 V below the negative supply.
The full-wave and half-wave rectifier shown in Figure 45
operates as follows: when V
IN
is above ground, R1 is boot-
strapped through the unity-gain follower A1 and the loop of
Amplifier A2. This forces the inputs of A2 to be equal, thus no
current flows through R1 or R2, and the circuit output tracks
the input. When V
IN
is below ground, the output of A1 is forced
to ground. The noninverting input of Amplifier A2 sees the
ground level output of A1; therefore, A2 operates as a unity-
gain inverter. The output at Node C is then a full-wave rectified
version of the input. Node B is a buffered half-wave rectified
version of the input. Input voltage supply to ±18 V can be
rectified, depending on the voltage supply used.
3
2
1
8
4
0.01µF
V
IN
+V
S
1/2
AD823
HALF-WAVE
RECTIFIED OUTPUT
FULL-WAVE
RECTIFIED OUTPUT
A1
R2
100k
R1
100k
6
5
7
1/2
AD823
A2
A
B
C
A2
00901-044
Figure 45. Full-Wave and Half-Wave Rectifier
100
A
B
C
2V
200µs
2V
10
0%
00901-046
90
Figure 46. Single-Supply Half-Wave and Full-Wave Rectifier

AD823ARZ

Mfr. #:
Manufacturer:
Analog Devices Inc.
Description:
Precision Amplifiers 17MHz RR FET Input Dual
Lifecycle:
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