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EVAL-ADM1026EB Datasheet(PDF) 20 Page - Analog Devices |
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EVAL-ADM1026EB Datasheet(HTML) 20 Page - Analog Devices |
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20 / 56 page ![]() ADM1026 Rev. A | Page 20 of 56 If the VREF output is not being used, it should be left uncon- nected. Do not connect VREF to GND using a capacitor. The internal output buffer on the voltage reference is capacitively loaded, which can cause the voltage reference to oscillate. This affects temperature readings reported back by the ADM1026. The recommended interface circuit for the VREF output is shown in Figure 33. 10k Ω 0.1 µF ADM1026 24 +12V 0.1 µF 10 µF 50 Ω VREF NDT3055 VREF Figure 33. VREF Interface Circuit for VREF Loads > 2 mA TEMPERATURE MEASUREMENT SYSTEM Local Temperature Measurement The ADM1026 contains an on-chip band gap temperature sensor whose output is digitized by the on-chip ADC. The temperature data is stored in the local temperature value register (Address 1Fh). As both positive and negative temper- atures can be measured, the temperature data is stored in twos complement format, as shown in Table 7. Theoretically, the temperature sensor and ADC can measure temperatures from −128°C to +127°C with a resolution of 1°C. Temperatures below TMIN and above TMAX are outside the operating temperature range of the device, however, so local temperature measure- ments outside this range are not possible. Temperature measurement from −128°C to +127°C is possible using a remote sensor. Remote Temperature Measurement The ADM1026 can measure the temperature of two remote diode sensors, or diode-connected transistors, connected to Pins 25 and 26, or 27 and 28. Pins 25 and 26 are a dedicated temperature input channel. Pins 27 and 28 can be configured to measure a diode sensor by clearing Bit 3 of Configuration Register 1 (Address 00h) to 0. If this bit is 1, then Pins 27 and 28 are AIN8 and AIN9. The forward voltage of a diode or diode-connected transistor, operated at a constant current, exhibits a negative temperature coefficient of about −2 mV/°C. Unfortunately, the absolute value of Vbe varies from device to device, and individual calibration is required to null this out, so the technique is unsuitable for mass production. The technique used in the ADM1026 is to measure the change in Vbe when the device is operated at two different currents, given by () N n q T K V be log Δ × × = where K is Boltzmann’s constant, q is the charge on the carrier, T is the absolute temperature in Kelvins, and N is the ratio of the two currents. Figure 34 shows the input signal conditioning used to measure the output of a remote temperature sensor. This figure shows the external sensor as a substrate transistor provided for temperature monitoring on some microprocessors, but it could equally well be a discrete transistor such as a 2N3904. If a discrete transistor is used, the collector is not grounded and should be linked to the base. If a PNP transistor is used, the base is connected to the D− input and the emitter to the D+ input. If an NPN transistor is used, the emitter is connected to the D− input and the base to the D+ input. To prevent ground noise from interfering with the measure- ment, the more negative terminal of the sensor is not referenced to ground but is biased above ground by an internal diode at the D− input. To measure ΔVbe, the sensor is switched between operating currents of I and N × I. The resulting waveform is passed through a 65 kHz low-pass filter to remove noise, and to a chopper-stabilized amplifier that performs the functions of amplification and rectification of the waveform to produce a DC voltage proportional to ΔVbe. This voltage is measured by the ADC to give a temperature output in 8-bit, twos complement format. To further reduce the effects of noise, digital filtering is performed by averaging the results of 16 measurement cycles. A remote temperature measurement takes nominally 2.14 ms. |
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