AD210JN

AD210
REV. A
–3–
INSIDE THE AD210
The AD210 basic block diagram is illustrated in Figure 1.
A +15 V supply is connected to the power port, and
±15 V isolated power is supplied to both the input and
output ports via a 50 kHz carrier frequency. The uncom-
mitted input amplifier can be used to supply gain or buff-
ering of input signals to the AD210. The fullwave
modulator translates the signal to the carrier frequency for
application to transformer T1. The synchronous demodu-
lator in the output port reconstructs the input signal. A
20 kHz, three-pole filter is employed to minimize output
noise and ripple. Finally, an output buffer provides a low
impedance output capable of driving a 2 k load.
INPUT
POWER
SUPPLY
19
14
15
16
17
18
V
O
30
29
T2
POWER
POWER
OSCILLATOR
INPUT OUTPUT
MOD
DEMOD
FILTER
1
2
OUTPUT
POWER
SUPPLY
3
4
O
COM
+V
OSS
–V
OSS
AD210
PWR COMPWR
T3
T1
–V
ISS
+V
ISS
I
COM
+IN
–IN
FB
Figure 1. AD210 Block Diagram
USING THE AD210
The AD210 is very simple to apply in a wide range of ap-
plications. Powered by a single +15 V power supply, the
AD210 will provide outstanding performance when used
as an input or output isolator, in single and multichannel
configurations.
Input Configurations: The basic unity gain configura-
tion for signals up to ±10 V is shown in Figure 2. Addi-
tional input amplifier variations are shown in the following
figures. For smaller signal levels Figure 3 shows how to
obtain gain while maintaining a very high input impedance.
19
14
15
16
17
18
V
OUT
(±10V)
30
29
+V
OSS
V
SIG
±10V
AD210
+V
ISS
–V
ISS
+15V
2
3
4
–V
OSS
1
V
OUT
Figure 2. Basic Unity Gain Configuration
The high input impedance of the circuits in Figures 2 and
3 can be maintained in an inverting application. Since the
AD210 is a three-port isolator, either the input leads or
the output leads may be interchanged to create the signal
inversion.
19
14
15
16
17
18
30
29
+V
OSS
V
SIG
AD210
+V
ISS
–V
ISS
+15V
2
3
4
–V
OSS
1
V
OUT
= V
SIG
1+
( )
R
F
R
G
R
G
R
F
Figure 3. Input Configuration for G > 1
Figure 4 shows how to accommodate current inputs or sum cur-
rents or voltages. This circuit configuration can also be used for
signals greater than ±10 V. For example, a ±100 V input span
can be handled with R
F
= 20 k and R
S1
= 200 k.
19
14
15
16
17
18
30
29
+V
OSS
AD210
+V
ISS
–V
ISS
+15V
2
3
4
–V
OSS
1
R
S1
I
S
V
S2
V
S1
R
S2
R
F
V
OUT
V
OUT
= –R
F
V
S1
R
S1
( )
V
S2
R
S2
+
+ I
S
+ ...
Figure 4. Summing or Current Input Configuration
Adjustments
When gain and offset adjustments are required, the actual cir-
cuit adjustment components will depend on the choice of input
configuration and whether the adjustments are to be made at
the isolator’s input or output. Adjustments on the output side
might be used when potentiometers on the input side would
represent a hazard due to the presence of high common-mode
voltage during adjustment. Offset adjustments are best done at
the input side, as it is better to null the offset ahead of the gain.
Figure 5 shows the input adjustment circuit for use when the in-
put amplifier is configured in the noninverting mode. This offset
adjustment circuit injects a small voltage in series with the
Figure 5. Adjustments for Noninverting Input
AD210
REV. A
–4–
low side of the signal source. This will not work if the source has
another current path to input common or if current flows in the
signal source LO lead. To minimize CMR degradation, keep the
resistor in series with the input LO below a few hundred ohms.
Figure 5 also shows the preferred gain adjustment circuit. The
circuit shows R
F
of 50 k, and will work for gains of ten or
greater. The adjustment becomes less effective at lower gains
(its effect is halved at G = 2) so that the pot will have to be a
larger fraction of the total R
F
at low gain. At G = 1 (follower)
the gain cannot be adjusted downward without compromising
input impedance; it is better to adjust gain at the signal source
or after the output.
Figure 6 shows the input adjustment circuit for use when the
input amplifier is configured in the inverting mode. The offset
adjustment nulls the voltage at the summing node. This is pref-
erable to current injection because it is less affected by subse-
quent gain adjustment. Gain adjustment is made in the feedback
and will work for gains from 1 V/V to 100 V/V.
19
15
16
17
18
30
29
+V
OSS
AD210
+V
ISS
–V
ISS
+15V
2
3
4
–V
OSS
V
OUT
V
SIG
14
200
47.5k
5k
100k
GAIN
OFFSET
50k
R
S
1
Figure 6. Adjustments for Inverting Input
Figure 7 shows how offset adjustments can be made at the out-
put, by offsetting the floating output port. In this circuit, ±15 V
would be supplied by a separate source. The AD210’s output
amplifier is fixed at unity, therefore, output gain must be made
in a subsequent stage.
19
15
16
17
18
30
29
+V
OSS
AD210
+V
ISS
–V
ISS
+15V
2
3
4
–V
OSS
V
OUT
14
200
1
0.1µF
100k
OFFSET
50k
+15V
–15V
Figure 7. Output-Side Offset Adjustment
PCB Layout for Multichannel Applications: The unique
pinout positioning minimizes board space constraints for multi-
channel applications. Figure 8 shows the recommended printed
circuit board layout for a noninverting input configuration with
gain.
R
F
R
G
R
F
R
G
R
F
R
G
POWER
CHANNEL INPUTS
1
2
3
0.1"
GRID
CHANNEL OUTPUTS
1
2
3
Figure 8. PCB Layout for Multichannel Applications with
Gain
Synchronization: The AD210 is insensitive to the clock of an
adjacent unit, eliminating the need to synchronize the clocks.
However, in rare instances channel to channel pick-up may
occur if input signal wires are bundled together. If this happens,
shielded input cables are recommended.
PERFORMANCE CHARACTERISTICS
Common-Mode Rejection: Figure 9 shows the common-
mode rejection of the AD210 versus frequency, gain and input
source resistance. For maximum common-mode rejection of
unwanted signals, keep the input source resistance low and care-
fully lay out the input, avoiding excessive stray capacitance at
the input terminals.
180
140
40
10 20 50 60 100 200 500 1k 2k 5k 10k
160
100
120
60
80
FREQUENCY – Hz
R
LO
= 0
R
LO
= 500
R
LO
= 0
R
LO
= 10k
R
LO
= 10k
G = 100
G = 1
CMR – dB
Figure 9. Common-Mode Rejection vs. Frequency
AD210
REV. A
–5–
+0.04
+0.03
+0.02
+0.01
0
–0.01
–0.02
–0.03
–0.04
–10 –8 –6 –4 –2 0 +2 +4 +6 +8 +10
OUTPUT VOLTAGE SWING – Volts
+8
+6
+4
+2
0
–2
–4
–6
–8
ERROR – mV
ERROR – %
Figure 12. Gain Nonlinearity Error vs. Output
0.01
0.009
0.008
0.007
0.006
0.005
0.004
0.003
0.002
0.001
0.000
100
90
80
70
60
50
40
30
20
10
0
0 2 4 6 8 10 12 14 16 18 20
TOTAL SIGNAL SWING – Volts
ERROR – % of Signal Swing
ERROR – ppm of Signal Swing
Figure 13. Gain Nonlinearity vs. Output Swing
Gain vs. Temperature: Figure 14 illustrates the AD210’s
gain vs. temperature performance. The gain versus temperature
performance illustrated is for an AD210 configured as a unity
gain amplifier.
400
200
0
–200
–400
–600
–800
–1000
–1200
–1400
–1600
–25 0 +25 +50 +70 +85
TEMPERATURE – °C
GAIN ERROR – ppm of Span
G = 1
Figure 14. Gain vs. Temperature
Phase Shift: Figure 10 illustrates the AD210’s low phase shift
and gain versus frequency. The AD210’s phase shift and wide
bandwidth performance make it well suited for applications like
power monitors and controls systems.
60
20
–80
100 100k10k1k10
40
–20
0
–60
–40
FREQUENCY – Hz
0
–20
–40
–60
–80
–100
–120
–140
PHASE SHIFT – Degrees
GAIN – dB
φG = 1
φG = 100
Figure 10. Phase Shift and Gain vs. Frequency
Input Noise vs. Frequency: Voltage noise referred to the input
is dependent on gain and signal bandwidth. Figure 11 illustrates
the typical input noise in nV/
Hz of the AD210 for a frequency
range from 10 to 10 kHz.
60
40
0
100 10k1k10
50
20
30
10
FREQUENCY – Hz
NOISE – nV/
Hz
Figure 11. Input Noise vs. Frequency
Gain Nonlinearity vs. Output: Gain nonlinearity is defined as the
deviation of the output voltage from the best straight line, and is
specified as % peak-to-peak of output span. The AD210B provides
guaranteed maximum nonlinearity of ±0.012% with an output span of
±10 V. The AD210’s nonlinearity performance is shown in Figure 12.
Gain Nonlinearity vs. Output Swing: The gain nonlinearity
of the AD210 varies as a function of total signal swing. When
the output swing is less than 20 volts, the gain nonlinearity as a
fraction of signal swing improves. The shape of the nonlinearity
remains constant. Figure 13 shows the gain nonlinearity of the
AD210 as a function of total signal swing.

AD210JN

Mfr. #:
Manufacturer:
Analog Devices Inc.
Description:
Isolation Amplifiers 120 kHz Bandwidth Iso AMP IC
Lifecycle:
New from this manufacturer.
Delivery:
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