AD8209 Data Sheet
Rev. C | Page 12 of 16
APPLICATIONS INFORMATION
HIGH-SIDE CURRENT SENSING
WITH A LOW-SIDE SWITCH
In load control configurations for high-side current sensing with a
low-side switch, the PWM-controlled switch is ground referenced.
An inductive load (solenoid) connects to a power supply/battery.
A resistive shunt is placed between the switch and the load (see
Figure 24). An advantage of placing the shunt on the high side
is that the entire current, including the recirculation current, is
monitored because the shunt remains in the loop when the switch
is off. In addition, shorts to ground can be detected with the shunt
on the high side, enhancing the diagnostics of the control loop. In
this circuit configuration, when the switch is closed, the common-
mode voltage moves down to near the negative rail. When the
switch is opened, the voltage reversal across the inductive load
causes the common-mode voltage to be held one diode drop
above the battery by the clamp diode.
GND
NC
–IN
+IN
A1
+V
S
A2
OUT
AD8209
5V
INDUCTIVE
LOAD
SWITCH
SHUNT
CLAMP
DIODE
BATTERY
NC = NO CONNECT
08461-026
C
F
OUTPUT
+
Figure 24. Low-Side Switch
In cases where a high-side switch is used for PWM control of the
load current in an application, the AD8209 can be used as shown
in Figure 25. The recirculation current through the freewheeling
diode (clamp diode) is monitored through the shunt resistor. In
this configuration, the common-mode voltage in the application
drops below GND when the FET is switched off. The AD8209
operates down to −2 V, providing an accurate current measurement.
GND
NC
–IN
+IN
A1
+V
S
A2
OUT
AD8209
5V
INDUCTIVE
LOAD
SWITCH
SHUNT
CLAMP
DIODE
BATTE
RY
NC = NO CONNECT
08461-027
C
F
OUTPUT
+
Figure 25. High-Side Switch
HIGH-RAIL CURRENT SENSING
In the high-rail current-sensing configuration, the shunt resistor is
referenced to the battery. High voltage is present at the inputs of
the current-sense amplifier. When the shunt is battery referenced,
the AD8209 produces a linear ground-referenced analog output.
Additionally, the AD8214 can be used to provide an overcurrent
detection signal in as little as 100 ns (see Figure 26). This feature is
useful in high current systems where fast shutdown in overcurrent
conditions is essential.
AD8214
INDUCTIVE
LOAD
SWITCH
CLAMP
DIODE
BATTERY
SHUNT
C
F
5V
–IN
NCGND
OVERCURRENT
DETECTION (<100ns)
OUT
V
S
+IN
V
REG
NC
–IN
GND
A1
A2
+IN
V
S
NC
OUT
AD8209
1
2
3
4
8
7
6
5
8765
1234
+
08461-028
Figure 26. Battery-Referenced Shunt Resistor
LOW-SIDE CURRENT SENSING
In systems where low-side current sensing is preferable, the
AD8209 provides a simple, high accuracy, integrated solution. In
this configuration, the AD8209 rejects ground noise and offers high
input to output linearity, regardless of the differential input voltage.
08461-029
GND
NC
–IN
+IN
A1
+V
S
A2
OUT
AD8209
5V
INDUCTIVE
LOAD
SWITCH
SHUNT
CLAMP
DIODE
BATTERY
NC = NO CONNECT
C
F
OUTPUT
Figure 27. Ground-Referenced Shunt Resistor
Data Sheet AD8209
Rev. C | Page 13 of 16
4 mA to 20 mA Current Loop Receiver
The AD8209 can also be used in low current-sensing applica-
tions, such as the 4 mA to 20 mA current loop receiver shown
in Figure 28. In such applications, the relatively large shunt
resistor may degrade the common-mode rejection. Adding a
resistor of equal value on the low impedance side of the input
corrects this error.
GND
NC
–IN
+IN
A1
+V
S
A2
OUT
AD8209
5V
B
ATTE
R
Y
10Ω
1%
10Ω
1%
NC = NO CONNECT
08461-030
C
F
OUTPUT
+
Figure 28. 4 mA to 20 mA Current Loop Receiver
GAIN ADJUSTMENT
The default gain of the preamplifier and buffer are 7 V/V and
2 V/V, respectively, resulting in a composite gain of 14 V/V. With
the addition of external resistor(s) or trimmer(s), the gain can
be lowered, raised, or finely calibrated.
Gains Less than 14
Because the preamplifier has an output resistance of 100 kΩ, an
external resistor connected from Pin 3 and Pin 4 to GND decreases
the gain by the following factor (see Figure 29):
R
EXT
/(100 kΩ + R
EXT
)
GND
NC
–IN
+IN
A1
+V
S
A2
OUT
AD8209
5V
V
DIFF
V
CM
NC = NO CONNECT
08461-031
R
EXT
OUTPUT
GAIN =
14R
EXT
R
EXT
+ 100kΩ
R
EXT
= 100kΩ
GAIN
14 – GAIN
+
+
Figure 29. Adjusting for Gains Less than 14
The overall bandwidth is unaffected by changes in gain by using
this method, although there may be a small offset voltage due to
the imbalance in source resistances at the input to the buffer. In
many cases, this can be ignored, but if desired, the offset voltage can
be nulled by inserting a resistor in series with Pin 4. The resistor
used should be equal to 100 k minus the parallel sum of R
EXT
and 100 kΩ. For example, with R
EXT
= 100 kΩ (yielding a composite
gain of 7 V/V), the optional offset nulling resistor is 50 kΩ.
Gains Greater than 14
Connecting a resistor from the output of the buffer amplifier to
its noninverting input, as shown in Figure 30, increases the gain.
The gain is now multiplied by the factor
R
EXT
/(R
EXT
100 kΩ)
For example, it is doubled for R
EXT
= 200 k. Overall gains as
high as 50 are achievable in this way. Note that the accuracy of
the gain becomes critically dependent on the resistor value at
high gains. In addition, the effective input offset voltage at Pin 1
and Pin 8 (which is about six times the actual offset of A1) limits
the use of the part in high gain, dc-coupled applications.
GND
NC
–IN
+IN
A1
+V
S
A2
OUT
AD8209
5V
V
DIFF
V
CM
NC = NO CONNECT
08461-032
R
EXT
POINT X
(SEE TEXT)
OUTPUT
GAIN =
14R
EXT
R
EXT
– 100k
R
EXT
= 100k
GAIN
GAIN – 14
+
+
Figure 30. Adjusting for Gains Greater than 14
A small offset voltage arises 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 is
comparable to the specified offset range and therefore introduces
negligible skew. However, it can be essentially eliminated by the
addition of a resistor in series with the parallel combination of
R
EXT
and 100 kΩ (at point X in Figure 30) so the total resistance
is maintained at 100 k. For example, at a gain of 20, when R
EXT
= 332 kand the parallel combination of R
EXT
and 100 kis
77 kΩ, the series resistor placed at point X is 23 kΩ.
AD8209 Data Sheet
Rev. C | Page 14 of 16
GAIN TRIM
Figure 31 shows a method for incremental gain trimming by
using a trim potentiometer and an external resistor, R
EXT
.
The following approximation is useful for small gain ranges:
ΔG ≈ (10 MΩ ÷ R
EXT
)%
For example, using this equation, the adjustment range is ±2%
for R
EXT
= 5 MΩ and ±10% for R
EXT
= 1 MΩ.
GND
NC
–IN
+IN
A1
+V
S
A2
R
EXT
OUT
AD8209
5V
V
DIFF
V
CM
NC = NO CONNECT
08461-033
OUTPUT
GAIN TRIM
20kΩ MIN
+
+
Figure 31. Incremental Gain Trimming
Internal Signal Overload Considerations
When configuring the gain for values other than 14, the maximum
input voltage with respect to the supply voltage and ground must
be considered because either the preamplifier or the output buffer
reaches its full-scale output (V
S
0.1 V) with large differential
input voltages. The input of the AD8209 is limited to (V
S
− 0.1) ÷
7 for overall gains of ≤7 because the preamplifier, with its fixed
gain of 7 V/V, reaches its full-scale output before the output
buffer. For gains greater than 7, the swing at the buffer output
reaches its full scale first and then limits the AD8209 input to
(V
S
− 0.1) ÷ G, where G is the overall gain.
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 with
large spikes may have PARs of 10 or more.
When implementing a filter, the PAR should be considered so
that the output of the AD8209 preamplifier (A1) does not clip
before A2; otherwise, the nonlinearity would be averaged and
appear as an error at the output. To avoid this error, both amplifiers
should 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 by using
the features provided by the AD8209. 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 tying Pin 3 to Pin 4 and adding a capacitor from this
node to ground, as shown in Figure 32. If a resistor is added
across the capacitor to lower the gain, the corner frequency
increases; therefore, gain should be calculated using the parallel
sum of the resistor and 100 kΩ.
GND
NC
–IN
+IN
A1
+V
S
A2
OUT
AD8209
5V
V
DIFF
V
CM
C
F
NC = NO CONNECT
08461-034
OUTPUT
f
C
=
1
2πC10
5
C IN FARADS
+
+
Figure 32. Single-Pole, Low-Pass Filter Using the Internal 100 kΩ Resistor
If the gain is raised using a resistor, as shown in Figure 30, the
corner frequency is lowered by the same factor as the gain is raised.
Therefore, using a resistor of 200 kΩ (for which the gain would
be doubled), results in a corner frequency scaled to 0.796 Hz µF
(0.039 µF for a 20 Hz corner frequency).
GND
NC
–IN
+IN
A1
+V
S
A2
OUT
AD8209
5V
V
DIFF
V
CM
C
C
NC = NO CONNECT
08461-035
OUTPUT
f
C
(Hz) = 1/C(
µF)
255k
+
+
Figure 33. 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 33. This
configuration is a Sallen-Key form based on a ×2 amplifier. It is
useful to remember that a two-pole filter with a corner frequency
of f
2
and a single-pole filter with a corner frequency of f
1
have
the same attenuation, that is, 40 log (f
2
/f
1
), as shown in Figure 34.
Using the standard resistor value shown in Figure 33 and capacitors
of equal values, the corner frequency is conveniently scaled to
1 Hz µF (0.05 µF for a 20 Hz corner frequency). A maximal flat
response occurs when the resistor is lowered to 196 kΩ, scaling
the corner frequency to 1.145 Hz µF. The output offset is raised
by approximately 5 mV (equivalent to 250 µV at the input pins).

AD8209WBRMZ

Mfr. #:
Manufacturer:
Analog Devices Inc.
Description:
Current Sense Amplifiers High VTG Precision
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