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AD8639ARMZ-R2 数据表(PDF) 15 Page - Analog Devices |
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AD8639ARMZ-R2 数据表(HTML) 15 Page - Analog Devices |
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15 / 20 page ![]() AD8638/AD8639 Rev. C | Page 15 of 20 INFRARED SENSORS Infrared (IR) sensors, particularly thermopiles, are increasingly used in temperature measurement for applications as wide ranging as automotive climate control, human ear thermometers, home insulation analysis, and automotive repair diagnostics. The relatively small output signal of the sensor demands high gain with very low offset voltage and drift to avoid dc errors. If interstage ac coupling is used, as shown in Figure 52, low offset and drift prevent the output of the input amplifier from drifting close to saturation. The low input bias currents generate minimal errors from the output impedance of the sensor. Similar to pressure sensors, the very low amplifier drift with time and temperature eliminates additional errors once the system is calibrated at room temperature. The low 1/f noise improves SNR for dc measurements taken over periods often exceeding one-fifth of a second. Figure 52 shows a circuit that can amplify ac signals from 100 μV to 300 μV up to the 1 V to 3 V levels, with a gain of 10,000 for accurate analog-to-digital conversions. 5V TO 16V 100kΩ 10kΩ 5V TO 16V 100µV TO 300µV 100Ω TO BIAS VOLTAGE 10kΩ fC ≈ 1.6Hz IR DETECTOR 100kΩ 10µF 1/2 AD8639 1/2 AD8639 Figure 52. AD8639 Used as a Preamplifier for Thermopile PRECISION CURRENT SHUNT SENSOR A precision current shunt sensor benefits from the unique attributes of auto-zero amplifiers when used in a differencing configuration, as shown in Figure 53. Current shunt sensors are used in precision current sources for feedback control systems. They are also used in a variety of other applications, including battery fuel gauging, laser diode power measurement and control, torque feedback controls in electric power steering, and precision power metering. RS 0.1Ω SUPPLY I RL 100Ω 100kΩ C 5V TO 16V 100Ω 100kΩ C e = 1000 RS I = 100mV/mA AD8638 Figure 53. Low-Side Current Sensing In such applications, it is desirable to use a shunt with very low resistance to minimize the series voltage drop; this minimizes wasted power and allows the measurement of high currents while saving power. A typical shunt may be 0.1 Ω. At measured current values of 1 A, the output signal of the shunt is hundreds of millivolts, or even volts, and amplifier error sources are not critical. However, at low measured current values in the 1 mA range, the 100 μV output voltage of the shunt demands a very low offset voltage and drift to maintain absolute accuracy. Low input bias currents are also needed to prevent injected bias current from becoming a significant percentage of the measured current. High open-loop gain, CMRR, and PSRR help to maintain the overall circuit accuracy. With the extremely high CMRR of the AD8638/AD8639, the CMRR is limited by the resistor ratio matching. As long as the rate of change of the current is not too fast, an auto-zero amplifier can be used with excellent results. OUTPUT AMPLIFIER FOR HIGH PRECISION DACS The AD8638/AD8639 can be used as output amplifiers for a 16-bit high precision DAC in a unipolar configuration. In this case, the selected op amp needs to have very low offset voltage (the DAC LSB is 38 μV when operating with a 2.5 V reference) to eliminate the need for output offset trims. Input bias current (typically a few tens of picoamperes) must also be very low because it generates an additional offset error when multiplied by the DAC output impedance (approximately 6 kΩ). Rail-to-rail output provides full-scale output with very little error. Output impedance of the DAC is constant and code- independent, but the high input impedance of the AD8638/ AD8639 minimizes gain errors. The wide bandwidth of the amplifier also serves well in this case. The amplifier, with a settling time of 4 μs, adds another time constant to the system, increasing the settling time of the output. For example, see Figure 54. The settling time of the AD5541 is 1 μs. The combined settling time is approximately 4.1 μs, as can be derived from the following equation: () ( ) ()2 2 8638 AD t DAC t TOTAL t S S S + = AD5541/AD5542 ADR421 AD8638 DGND *AD5542 ONLY VDD VOUT REF(REFF*) REFS* SCLK DIN CS AGND 5V UNIPOLAR OUTPUT LDAC* 0.1µF 0.1µF 2.5V 62 4 0.1µF SERIAL INTERFACE 5V TO 16V 5V TO 16V Figure 54. AD8638 Used as an Output Amplifier |
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