AD822ARMZ Analog Devices Inc, AD822ARMZ Datasheet - Page 18
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AD822ARMZ
Manufacturer Part Number
AD822ARMZ
Description
DUAL, SNGL SPLY PRECN AMP
Manufacturer
Analog Devices Inc
Datasheet
1.AD822ARMZ-REEL.pdf
(24 pages)
Specifications of AD822ARMZ
Rohs Compliant
YES
Design Resources
16-Bit Fully Isolated 4 mA to 20 mA Output Module Using AD5662, ADuM1401, and External Amplifiers (CN0064)
Amplifier Type
General Purpose
Number Of Circuits
2
Output Type
Rail-to-Rail
Slew Rate
3 V/µs
Gain Bandwidth Product
1.9MHz
-3db Bandwidth
1.9MHz
Current - Input Bias
2pA
Voltage - Input Offset
400µV
Current - Supply
1.4mA
Current - Output / Channel
20mA
Voltage - Supply, Single/dual (±)
3 V ~ 36 V, ±1.5 V ~ 18 V
Operating Temperature
-40°C ~ 85°C
Mounting Type
Surface Mount
Package / Case
8-MSOP, Micro8™, 8-uMAX, 8-uSOP,
Op Amp Type
Low Power
No. Of Amplifiers
2
Bandwidth
1.8MHz
Supply Voltage Range
± 2.5V To ± 15V
Amplifier Case Style
MSOP
No. Of Pins
8
Lead Free Status / RoHS Status
Lead free / RoHS Compliant
Available stocks
Company
Part Number
Manufacturer
Quantity
Price
Company:
Part Number:
AD822ARMZ
Manufacturer:
Analog Devices Inc
Quantity:
30 790
Part Number:
AD822ARMZ
Manufacturer:
ADI/亚德诺
Quantity:
20 000
Company:
Part Number:
AD822ARMZ-REEL
Manufacturer:
AD
Quantity:
15 600
Part Number:
AD822ARMZ-REEL7
Manufacturer:
ADI/亚德诺
Quantity:
20 000
AD822
APPLICATIONS INFORMATION
INPUT CHARACTERISTICS
In the AD822, 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
Driving the input voltage closer to the positive rail causes a loss
of amplifier bandwidth (as can be seen by comparing the large
signal responses shown in Figure 34 and Figure 37) and increased
common-mode voltage error as illustrated in Figure 20.
The AD822 does not exhibit phase reversal for input voltages
up to and including +V
AD822 voltage follower to a 0 V to 5 V (+V
The input and output are superimposed. The output tracks the
input up to +V
above a 4 V input causes the rounding of the output waveform.
For input voltages greater than +V
AD822 noninverting input prevents phase reversal, at the expense
of greater input voltage noise. This is illustrated in Figure 42.
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
internal device junctions become forward biased. This is illu-
strated in Figure 7.
A current limiting resistor should be used in series with the input
of the AD822 if there is a possibility of the input voltage exceed-
ing the positive supply by more than 300 mV, or if an input voltage
is applied to the AD822 when +V
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 conti-
nuous overvoltage and increases the input voltage noise by a
negligible amount.
Input voltages less than −V
amplifier can safely withstand input voltages 20 V below the
negative supply voltage if the total voltage from the positive
supply to the input terminal is less than 36 V. In addition, the
input stage typically maintains picoampere (pA) level input
currents across that input voltage range.
The AD822 is designed for 13 nV/√Hz wideband input voltage
noise and maintains low noise performance to low frequencies
(refer to Figure 14). This noise performance, along with the
AD822 low input current and current noise, means that the
AD822 contributes negligible noise for applications with source
resistances greater than 10 kΩ and signal bandwidths greater
than 1 kHz. This is illustrated in Figure 43.
S
− 0.4 V, then the input current reverses direction as
S
without phase reversal. The reduced bandwidth
S
. Figure 42 shows the response of an
S
are a completely different story. The
S
S
or −V
, a resistor in series with the
S
S
= 0 V. The amplifier is
to 1 V less than +V
S
) square wave input.
Rev. I | Page 18 of 24
S
.
OUTPUT CHARACTERISTICS
The AD822 unique bipolar rail-to-rail output stage swings within
5 mV of the negative supply and 10 mV of the positive supply with
no external resistive load. The approximate output saturation
resistance of the AD822 is 40 Ω sourcing and 20 Ω sinking, which
can be used to estimate output saturation voltage when driving
heavier current loads. For instance, when sourcing 5 mA, the
saturation voltage to the positive supply rail is 200 mV; when
sinking 5 mA, the saturation voltage to the negative rail is 100 mV.
The open-loop gain characteristic of the amplifier changes as a
function of resistive load, as shown in Figure 10 to Figure 13.
For load resistances over 20 kΩ, the AD822 input error voltage
is virtually unchanged until the output voltage is driven to 180 mV
of either supply.
If the AD822 output is overdriven so that either of the output
devices are saturated, the amplifier recovers within 2 μs of its
input returning to the linear operating region of the amplifier.
Direct capacitive loads interact with the effective output imped-
ance of the amplifier to form an additional pole in the amplifier
feedback loop, which can cause excessive peaking on the pulse
response or loss of stability. The worst case occurs when the
amplifier is used as a unity-gain follower. Figure 44 shows the
AD822 pulse response as a unity-gain follower driving 350 pF.
This amount of overshoot indicates approximately 20° of phase
margin—the system is stable, but nearing the edge. Configurations
with less loop gain, and as a result less loop bandwidth, are
much less sensitive to capacitance load effects.
100k
10k
100
0.1
1k
10
1
10k
WHENEVER JOHNSON NOISE IS GREATER THAN
AMPLIFIER NOISE, AMPLIFIER NOISE CAN BE
CONSIDERED NEGLIGIBLE FOR APPLICATION.
Figure 43. Total Noise vs. Source Impedance
100k
RESISTOR JOHNSON
NOISE
SOURCE IMPEDANCE (Ω)
1M
10M
AMPLIFIER-GENERATED
NOISE
100M
1kHz
1G
10Hz
10G