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ADT14GS датащи(PDF) 12 Page - Analog Devices |
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ADT14GS датащи(HTML) 12 Page - Analog Devices |
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12 / 16 page ![]() ADT14 –12– REV. 0 By connecting the VPTAT output to the input of the AD654, the 5 mV/K, temperature coefficient gives a sensitivity of 25 Hz/ °C, centered around 7.5 kHz at 25°C. The trimming resistor, R2, is needed to calibrate the absolute accuracy of the AD654. For more information on the converter, consult the AD654 data sheet. An AD650 frequency-to-voltage converter can be used to accurately convert the frequency back to a dc voltage on the receiving end. OSC AD654 86 7 1 4 3 52 V+ C1 0.1 F 5k Ω V+ FOUT R1 1.8k Ω R2 500 Ω ADT14 VPTAT Figure 23. Temperature-to-Frequency Converter Isolation Amplifier In many industrial applications the sensor is located in an envi- ronment that needs to be electrically isolated from the central processing area. Figure 24 shows a simple circuit that uses an 8-pin opto-isolator (IL300XC) that can operate across a 5,000 V barrier. IC1 (an OP290 single-supply amplifier) is used to drive the LED connected between Pins 1 to 2. The feedback actually comes from the photodiode connected to Pins 3 to 4. The OP290 drives the LED such that there is enough current generated in the photodiode to exactly equal the current derived from the VPTAT voltage across the 470 k Ω resistor. On the receiving end, an OP90 converts the current from the second photodiode to a voltage through its feedback resistor R2. Note that the other amplifier in the dual OP290 is used to buffer the 2.5 V reference voltage of the ADT14 for an accurate, low drift LED bias level without affecting the programmed hysteresis current. A REF43 (a precision 2.5 V reference) provides an accurate bias level at the receiving end. To understand this circuit, it helps to examine the overall equa- tion for the output voltage. First, the current (I1) in the photo- diode is set by: I1 = 2.5V –VPTAT 470 k Ω Note that the IL300XC has a gain of 0.73 (typical) with a min and max of 0.693 and 0.769 respectively. Since this is less than 1.0, R2 must be larger than R1 to achieve overall unity gain. To show this the full equation is: VOUT = 2.5V – I2R2 = 2.5V –0.7 2.5V –VPTAT 470 k Ω ×644 kΩ=VPTAT A trim is included for R2 to correct for the initial gain accuracy of the IL300XC. To perform this trim, simply adjust for an output equal to VPTAT at any particular temperature. For example, at room temperature, VPTAT = 1.49 V, so adjust R2 until VOUT = 1.49 V as well. Both the REF43 and the OP90 operate from a single supply, and contribute no significant error due to drift. In order to avoid the accuracy trim, and to reduce board space, complete isolation amplifiers, such as the high accuracy AD202, are available. OP290 OP290 V+ ADT14 VREF VPTAT 60µF 100 Ω IN9148 I1 I2 IL300XC 1 2 3 4 OP90 ISOLATION BARRIER V+ 2.5V 6 2 4 V+ 604k Ω 100k Ω 680pF 1.16V TO 1.7V R1 470k Ω REF43 Figure 24. Isolation Amplifier |
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