AD8132ARM Analog Devices Inc, AD8132ARM Datasheet - Page 29

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AD8132ARM

Manufacturer Part Number
AD8132ARM
Description
Amplifier IC
Manufacturer
Analog Devices Inc
Datasheet

Specifications of AD8132ARM

Bandwidth
350MHz
Slew Rate
1200V/µs
No. Of Pins
8
Operating Temperature Range
-40°C To +85°C
Peak Reflow Compatible (260 C)
No
Leaded Process Compatible
No
Mounting Type
Surface Mount
Package / Case
8-uSOIC
Rohs Status
RoHS non-compliant
Amplifier Type
Differential
Number Of Circuits
1
Output Type
Differential
-3db Bandwidth
360MHz
Current - Input Bias
3µA
Voltage - Input Offset
1000µV
Current - Supply
12mA
Current - Output / Channel
70mA
Voltage - Supply, Single/dual (±)
2.7 V ~ 11 V, ±1.35 V ~ 5.5 V
Operating Temperature
-40°C ~ 125°C
Lead Free Status / RoHS Status
Contains lead / RoHS non-compliant
Gain Bandwidth Product
-
Lead Free Status / RoHS Status
Contains lead / RoHS non-compliant

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FULL-WAVE RECTIFIER
The balanced outputs of the AD8132, along with a couple of
Schottky diodes, can create a very high speed, full-wave rectifier.
Such circuits are useful for measuring ac voltages and other
computational tasks.
Figure 82 shows the configuration of such a circuit. Each of the
AD8132 outputs drives the anode of an HP2835 Schottky diode.
These Schottky diodes were chosen for their high speed operation.
At lower frequencies (approximately lower than 10 MHz), a silicon
signal diode, such as a 1N4148, can be used. The cathodes of the
two diodes are connected together, and this output node is
connected to ground by a 100 Ω resistor.
Operate the diodes such that they are slightly forward-biased
when the differential output voltage is zero. For the Schottky
diodes, this is approximately 400 mV. The forward biasing is
conveniently adjusted by CR1, which, in this circuit, raises and
lowers V
One advantage of this circuit is that the feedback loop is never
momentarily opened while the diodes reverse their polarity within
the loop. This scheme is sometimes used for full-wave rectifiers
that use conventional op amps. These conventional circuits do
not work well at frequencies above approximately 1 MHz.
V
IN
49.9Ω
OUT, cm
R
T1
24.9Ω
without creating a differential output voltage.
R
T2
10kΩ
+5V
Figure 82. Full-Wave Rectifier
348Ω
348Ω
R
R
G1
G2
CR1
+5V
–5V
348Ω
348Ω
R
R
F2
F1
R
100Ω
L
HP2835
V
OUT
Rev. I | Page 29 of 32
If there is not enough forward bias (V
sharp cusps of the full-wave rectified output waveform are rounded
off. In addition, as the frequency increases, there tends to be some
rounding of the lower cusps. The forward bias can be increased
to yield sharper cusps at higher frequencies.
There is not a reliable, entirely quantifiable, means to measure
the performance of a full-wave rectifier. Because the ideal
waveform has periodic sharp discontinuities, it has (mostly
even) harmonics that have no upper bound on the frequency.
However, for a practical circuit, as the frequency increases, the
higher harmonics become attenuated and the sharp cusps that
are present at low frequencies become significantly rounded.
When running the circuit at a frequency up to 300 MHz, though it
stays functional, the major harmonic that remains in the output
is the second. This looks like a sine wave at 600 MHz. Figure 83 is
an oscilloscope plot of the output when driven by a 100 MHz,
2.5 V p-p input.
Sometimes a second harmonic generator is useful for creating a
clock to oversample a DAC by a factor of two. If the output of
this circuit is run through a low-pass filter, it can be used as a
second harmonic generator.
AUTOMOTIVE PRODUCTS
The AD8132W is qualified per the AEC-Q100 for use in
automotive applications. Custom variants of this product may
be available to meet stringent automotive performance and
quality requirements.
Figure 83. Full-Wave Rectifier Response with 100 MHz Input
100mV
1V
OUT, cm
2ns
too low), the lower
AD8132

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