OP184FSZ-REEL7 Analog Devices Inc, OP184FSZ-REEL7 Datasheet - Page 20

IC OPAMP GP R-R 4.25MHZ LN 8SOIC

OP184FSZ-REEL7

Manufacturer Part Number
OP184FSZ-REEL7
Description
IC OPAMP GP R-R 4.25MHZ LN 8SOIC
Manufacturer
Analog Devices Inc
Datasheet

Specifications of OP184FSZ-REEL7

Slew Rate
4 V/µs
Design Resources
Variable Gain Noninverting Amplifier Using AD5292 and OP184 (CN0112) Variable Gain Inverting Amplifier Using AD5292 and OP184 (CN0113) Programmable High Voltage Source with Boosted Output Current Using AD5292, OP184, and MOSFETs (CN0115) Low-Noise Microwave fractional-N PLL using active loop filter and RF prescaler (CN0174)
Amplifier Type
General Purpose
Number Of Circuits
1
Output Type
Rail-to-Rail
Gain Bandwidth Product
4.25MHz
Current - Input Bias
80nA
Voltage - Input Offset
175µV
Current - Supply
2.25mA
Current - Output / Channel
10mA
Voltage - Supply, Single/dual (±)
3 V ~ 36 V, ±1.5 V ~ 18 V
Operating Temperature
-40°C ~ 125°C
Mounting Type
Surface Mount
Package / Case
8-SOIC (3.9mm Width)
Op Amp Type
Precision
No. Of Amplifiers
1
Bandwidth
4.25MHz
Supply Voltage Range
± 1.5V To ± 18V
Amplifier Case Style
SOIC
No. Of Pins
8
Lead Free Status / RoHS Status
Lead free / RoHS Compliant
-3db Bandwidth
-
Lead Free Status / RoHS Status
Lead free / RoHS Compliant, Lead free / RoHS Compliant
OP184/OP284/OP484
Obviously, it is desirable to keep this comparison voltage small
because it becomes a significant portion of the overall dropout
voltage. Here, the 20 mV reference is higher than the typical
offset of the OP284 but is still reasonably low as a percentage
of V
Sense Resistor R
maintain this threshold voltage between 20 mV and 50 mV.
Performance of the circuit is excellent. For the 4.5 V output
version, the measured dc output change for a 225 mA load
change was on the order of a few microvolts, while the dropout
voltage at this same current level was about 30 mV. The current
limit, as shown in Figure 58, is 400 mA, allowing the circuit to
be used at levels up to 300 mA or more. While the Q1 device can
actually support currents of several amperes, a practical current
rating takes into account the 2.5 W, 25°C dissipation of the
8-lead SOIC device. Because a short-circuit current of 400 mA
at an input level of 5 V causes a 2 W dissipation in Q1, other input
conditions must be considered carefully in terms of potential
overheating of Q1. Of course, if higher powered devices are used
for Q1, this circuit can support outputs of tens of amperes as
well as the higher V
The circuit shown can either be used as a standard low dropout
regulator, or it can be used with on/off control. By driving Pin 3
of U2 with the optional logic control signal, V
switched between on and off. Note that when the output is off
in this circuit, it is still active (that is, not an open circuit). This
is because the off state simply reduces the voltage input to R1,
leaving the U1A/U1B amplifiers and Q1 still active.
When the on/off control is used, Resistor R10 should be used
with U2 to speed on/off switching and to allow the output of the
circuit to settle to a nominal zero voltage. Component D3 and
Component R11 also aid in speeding up the on/off transition by
providing a dynamic discharge path for C2. Off/on transition
time is less than 1 ms, while the on/off transition is longer, but
less than 10 ms.
3 V, 50 HZ/60 HZ ACTIVE NOTCH FILTER WITH
FALSE GROUND
To process signals in a single-supply system, it is often best to use
a false ground biasing scheme. A circuit that uses this approach is
shown in Figure 59. In this circuit, a false ground circuit biases
an active notch filter used to reject 50 Hz/60 Hz power line
interference in portable patient monitoring equipment.
OUT
(<0.5%). In adapting the limiter for other I
S
should be adjusted along with R7 to R8, to
OUT
levels already noted.
C
, the output is
LIMIT
levels,
Rev. I | Page 20 of 24
Notch filters are commonly used to reject power line frequency
interference that often obscures low frequency physiological
signals, such as heart rates, blood pressure readings, EEGs, and
EKGs. This notch filter effectively squelches 60 Hz pickup at a
Filter Q of 0.75. Substituting 3.16 kΩ resistors for the 2.67 kΩ
resistor in the twin-T section (R1 through R5) configures the
active filter to reject 50 Hz interference.
Amplifier A3 is the heart of the false ground bias circuit. It buffers
the voltage developed at R9 and R10 and is the reference for the
active notch filter. Because the OP484 exhibits a rail-to-rail input
common-mode range, R9 and R10 are chosen to split the 3 V
supply symmetrically. An in-the-loop compensation scheme is
used around the OP484 that allows the op amp to drive C6, a
1 μF capacitor, without oscillation. C6 maintains a low impedance
ac ground over the operating frequency range of the filter.
The filter section uses an OP484 in a Twin-T configuration whose
frequency selectivity is very sensitive to the relative matching of
the capacitors and resistors in the twin-T section. Mylar is the
material of choice for the capacitors, and the relative matching
of the capacitors and resistors determines the pass band symmetry
of the filter. Using 1% resistors and 5% capacitors produces satis-
factory results.
V
IN
1µF
C4
Figure 59. A 3 V Single-Supply, 50Hz to 60 Hz Active Notch Filter
R6
10kΩ
3V
2
3
R9
20kΩ
R10
20kΩ
A1
3V
11
4
2.67kΩ
10
1
9
R1
A1, A2, A3 = OP484
A3
0.03µF
(1µF × 2)
C5
2.67kΩ
2µF
R3
1µF
10kΩ
C1
C3
R11
8
with False Ground
150Ω
R12
2.67kΩ
R5
1.33kΩ
(2.68kΩ ÷ 2)
1µF
R4
C2
NOTE: FOR 50Hz APPLICATIONS
Q = 0.75
C6
1µF
1.5V
2.67kΩ
CHANGE R1, R2, R3, AND R4 TO 3.1kΩ
AND R5 TO 1.58kΩ (3.16kΩ ÷ 2).
R2
R8
1kΩ
5
6
A2
1kΩ
R7
7
V
O

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