OP295 Datasheet, PDF (10/12 Pages) Analog Devices – DUAL/QUAD RAIL-TO-RAIL OPERATIONAL AMPLIFIERS

OP295/OP495
current budget with which the circuit must operate. This circuit
consumes only 1.4 mA maximum quiescent current, making 2.6
mA of current available to power additional signal conditioning
circuitry or to power a bridge circuit.
A 3 Volt Low-Dropout Linear Voltage Regulator
Figure 10 shows a simple 3 V voltage regulator design. The
regulator can deliver 50 mA load current while allowing a 0.2 V
dropout voltage. The OP295/OP495’s rail-to-rail output swing
handily drives the MJE350 pass transistor without requiring spe-
cial drive circuitry. At no load, its output can swing less than the
pass transistor’s base-emitter voltage, turning the device nearly
off. At full load, and at low emitter-collector voltages, the tran-
sistor beta tends to decrease. The additional base current is eas-
ily handled by the OP295/OP495 output.
The amplifier servos the output to a constant voltage, which
feeds a portion of the signal to the error amplifier.
Higher output current, to 100 mA, is achievable at a higher
dropout voltage of 3.8 V.
V_IN
5V TO 3.2V
MJE 350
8
3
1/2
1 OP295/
OP495
4
2
1000pF
43k
I_L < 50mA
V_O
44.2k
1%
100µF
30.9k
1%
1.235V
AD589
Figure 10. 3 V Low Dropout Voltage Regulator
Figure 11 shows the regulator’s recovery characteristic when its
output underwent a 20 mA to 50 mA step current change.
2V
100
50mA 90
STEP
CURRENT
CONTROL
WAVEFORM
20mA
OUTPUT
10
0%
20mV
1ms
Figure 11. Output Step Load Current Recovery
Low-Dropout, 500 mA Voltage Regulator with Fold-Back
Current Limiting
Adding a second amplifier in the regulation loop as shown in
Figure 12 provides an output current monitor as well as fold-
back current limiting protection.
Amplifier A1 provides error amplification for the normal voltage
regulation loop. As long as the output current is less than 1 am-
pere, amplifier A2’s output swings to ground, reverse biasing the
diode and effectively taking itself out of the circuit. However, as
the output current exceeds 1 amp, the voltage that develops
across the 0.1 Ω sense resistor forces the amplifier A2’s output
to go high, forward-biasing the diode, which in turn closes the
current limit loop. At this point A2’s lower output resistance
dominates the drive to the power MOSFET transistor, thereby
effectively removing the A1 voltage regulation loop from the
circuit.
If the output current greater than 1 amp persists, the current
limit loop forces a reduction of current to the load, which causes
a corresponding drop in output voltage. As the output voltage
drops, the current limit threshold also drops fractionally, result-
ing in a decreasing output current as the output voltage de-
creases, to the limit of less than 0.2 A at 1 V output. This
“fold-back” effect reduces the power dissipation considerably
during a short circuit condition, thus making the power supply
far more forgiving in terms of the thermal design requirements.
Small heat sinking on the power MOSFET can be tolerated.
The OP295’s rail-to-rail swing exacts higher gate drive to
the power MOSFET, providing a fuller enhancement to the
transistor. The regulator exhibits 0.2 V dropout at 500 mA of
load current. At 1 amp output, the dropout voltage is typically
5.6 volts.
IRF9531
SD
6V
G
R_SENSE
0.1Ω
1/4W
210k
1%
I_O (NORM) = 0.5A
I_O (MAX) = 1A
205k
1%
+5V V_O
85
7 A2
1N4148
1/2
6
OP295/
OP495
100k
5%
0.01µF
3
1 A1
1/2 4 ₂
OP295/
OP495
REF43
2
6
4
45.3k
1%
124k
1%
2.500V
45.3k
1%
124k
1%
Figure 12. Low Dropout, 500 mA Voltage Regulator with
Fold-Back Current Limiting
Square Wave Oscillator
The circuit in Figure 13 is a square wave oscillator (note the
positive feedback). The rail-to-rail swing of the OP295/OP495
helps maintain a constant oscillation frequency even if the sup-
ply voltage varies considerably. Consider a battery powered sys-
tem where the voltages are not regulated and drop over time.
The rail-to-rail swing ensures that the noninverting input sees
the full V+/2, rather than only a fraction of it.
The constant frequency comes from the fact that the 58.7 kΩ
feedback sets up Schmitt Trigger threshold levels that are di-
rectly proportional to the supply voltage, as are the RC charge
voltage levels. As a result, the RC charge time, and therefore the
frequency, remains constant independent of supply voltage. The
slew rate of the amplifier limits the oscillation frequency to a
maximum of about 800 Hz at a +5 V supply.
Single Supply Differential Speaker Driver
Connected as a differential speaker driver, the OP295/OP495
can deliver a minimum of 10 mA to the load. With a 600 Ω
load, the OP295/OP495 can swing close to 5 volts peak-to-peak
across the load.
–10–
REV. B