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OP193FSZ 数据表(PDF) 15 Page - Analog Devices |
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OP193FSZ 数据表(HTML) 15 Page - Analog Devices |
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15 / 20 page ![]() OP193/OP293 Rev. C | Page 15 of 20 A MICROPOWER FALSE-GROUND GENERATOR Some single-supply circuits work best when inputs are biased above ground, typically at ½ of the supply voltage. In these cases, a false ground can be created by using a voltage divider buffered by an amplifier. One such circuit is shown in Figure 30. This circuit generates a false-ground reference at ½ of the supply voltage, while drawing only about 27 μA from a 5 V supply. The circuit includes compensation to allow for a 1 μF bypass capacitor at the false-ground output. The benefit of a large capacitor is that not only does the false ground present a very low dc resistance to the load, but its ac impedance is low as well. The OP193 can both sink and source more than 5 mA, which improves recovery time from transients in the load current. OP193 2 3 6 7 5V OR 12V 2.5V OR 6V + + 4 10k Ω 100 Ω 0.022µF 240k Ω 240k Ω 1µF 1µF Figure 30. A Micropower False-Ground Generator A BATTERY-POWERED VOLTAGE REFERENCE The circuit of Figure 31 is a battery-powered voltage reference that draws only 17 μA of supply current. At this level, two AA alkaline cells can power this reference for more than 18 months. At an output voltage of 1.23 V at 25°C, drift of the reference is only 5.5 μV/°C over the industrial temperature range. Load regulation is 85 μV/mA with line regulation at 120 μV/V. Design of the reference is based on the Brokaw band gap core technique. Scaling of Resistor R1 and Resistor R2 produces unequal currents in Q1 and Q2. The resulting ΔVBE across R3 creates a temperature-proportional voltage (PTAT), which, in turn, produces a larger temperature-proportional voltage across R4 and R5, V1. The temperature coefficient of V1 cancels (first order) the complementary to absolute temperature (CTAT) coefficient of VBE1. When adjusted to 1.23 V at 25°C, output voltage temperature coefficient is at a minimum. Band gap references can have start-up problems. With no current in R1 and R2, the OP193 is beyond its positive input range limit and has an undefined output state. Shorting Pin 5 (an offset adjust pin) to ground forces the output high under these circumstances and ensures reliable startup without significantly degrading the OP193’s offset drift. 3 OP193 2 4 5 6 7 VBE2 Q1 V+ (2.5V TO 36V) Q2 1 2 3 7 6 5 MAT01AH R3 68k Ω V1 R2 1.5M Ω VOUT (1.23V @ 25°C) C1 1000pF R1 240k Ω VBE1 + – + – + – ΔVBE R4 130k Ω R5, 20k Ω OUTPUT ADJUST Figure 31. A Battery-Powered Voltage Reference A SINGLE-SUPPLY CURRENT MONITOR Current monitoring essentially consists of amplifying the voltage drop across a resistor placed in series with the current to be measured. The difficulty is that only small voltage drops can be tolerated, and with low precision op amps, this greatly limits the overall resolution. The single-supply current monitor of Figure 32 has a resolution of 10 μA and is capable of monitoring 30 mA of current. This range can be adjusted by changing the current sense resistor, R1. When measuring total system current, it may be necessary to include the supply current of the current monitor, which bypasses the current sense resistor, in the final result. This current can be measured and calibrated (together with the residual offset) by adjustment of the offset trim potentiometer, R2. This produces a deliberate temperature dependent offset. However, the supply current of the OP193 is also proportional to temperature, and the two effects tend to track. Voltage devel- oped at the noninverting input and amplified by (1 + R4/R5) appears at VOUT. TO CIRCUIT UNDER TEST V+ OP193 3 2 1 5 6 4 7 + – VOUT = 100mV/mA(ITEST) R4 9.9k Ω R2 100k Ω ITEST R1 1 Ω R5 100 Ω R3 100k Ω Figure 32. Single-Supply Current Monitor |
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