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OP481GS 数据表(PDF) 12 Page - Analog Devices |
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OP481GS 数据表(HTML) 12 Page - Analog Devices |
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12 / 16 page ![]() OP181/OP281/OP481 –12– REV. 0 A1 R1 R2 +3V OP281-A VIN 2k Ω 5.1k Ω +3V +3V VOUT Q1 5.1k Ω VH D1 10k Ω A2 R3 R4 +3V +3V VL D2 OP281-B Figure 39. Using the OP281 as a Window Comparator The threshold limits for the window are set by VH and VL, provided that VH > VL. The output of A1 will stay at the negative rail, in this case ground, as long as the input voltage is less than VH. Similarly, the output of A2 will stay at ground as long the input voltage is higher than VL. As long as VIN remains between VL and VH, the outputs of both op amps will be 0 V. With no current flowing in either D1 or D2, the base of Q1 will stay at ground, putting the transistor in cutoff and forcing VOUT to the positive supply rail. If the input voltage rises above VH, the output of A2 stays at ground, but the output of A1 will go to the positive rail, and D1 will conduct current. This creates a base voltage that will turn on Q1 and drive VOUT low. The same condition occurs if VIN falls below VL with A2’s output going high, and D2 conducting current. Therefore, VOUT will be high if the input voltage is between VL and VH, and VOUT will be low if the input voltage moves outside of that range. The R1 and R2 voltage divider sets the upper window voltage, and the R3 and R4 voltage divider sets the lower voltage for the window. For the window comparator to function properly, VH must be a greater voltage than VL. VH = R2 R1 + R2 VL = R4 R3 + R4 The 2 k Ω resistor connects the input voltage to the input termi- nals to the op amps. This protects the OP281 from possible excess current flowing into the input stages of the devices. D1 and D2 are small-signal switching diodes (1N4446 or equiva- lent), and Q1 is a 2N2222 or equivalent NPN transistor. A Low-Side Current Monitor In the design of power supply control circuits, a great deal of design effort is focused on ensuring a pass transistor’s long-term reliability over a wide range of load current conditions. As a result, monitoring and limiting device power dissipation is of prime importance in these designs. Figure 40 shows an example of a +5 V, single-supply current monitor that can be incorpo- rated into the design of a voltage regulator with fold-back current limiting or a high current power supply with crowbar protection. The design capitalizes on the OP181’s common- mode range that extends to ground. Current is monitored in the power supply return path where a 0.1 Ω shunt resistor, R SENSE, creates a very small voltage drop. The voltage at the inverting terminal becomes equal to the voltage at the noninverting terminal through the feedback of Q1, which is a 2N2222 or equivalent NPN transistor. This makes the voltage drop across R1 equal to the voltage drop across RSENSE. Therefore, the current through Q1 becomes directly proportional to the current through RSENSE, and the output voltage is given by: VOUT = VEE − R2 R1 × R SENSE × I L The voltage drop across R2 increases with IL increasing, so VOUT decreases with higher supply current being sensed. For the element values shown, the VOUT transfer characteristic is –2.5 V/A, decreasing from VEE. +5V RETURN TO GROUND OP181 +5V R2 2.49k Ω VOUT R1 100 Ω 0.1 Ω RSENSE Q1 Figure 40. A Low-Side Load Current Monitor Low Voltage Half-Wave and Full-Wave Rectifiers Because of its quick overdrive recovery time, an OP281 can be configured as a full-wave rectifier for low frequency (<500 Hz) applications. Figure 41 shows the schematic. +3V OP281-A VIN = 2V p-p 2k Ω A1 +3V OP281-B A2 R1 = 100k Ω R2 = 100k Ω FULL-WAVE RECTIFIED OUTPUT HALF-WAVE RECTIFIED OUTPUT Figure 41. Single Supply Full- and Half-Wave Rectifiers Using an OP281 10 0% 100 90 SCALE 0.1V/DIV SCALE 0.1ms/DIV Figure 42. Full-Wave Rectified Signal |
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