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ADT7467ARQZ-R7 Datasheet(PDF) 17 Page - ON Semiconductor |
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ADT7467ARQZ-R7 Datasheet(HTML) 17 Page - ON Semiconductor |
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17 / 77 page ![]() ADT7467 Rev. 3 | Page 17 of 77 | www.onsemi.com Remote Temperature Measurement The ADT7467 can measure the temperature of two remote diode sensors or diode-connected transistors connected to Pin 10 and Pin 11 or to Pin 12 and Pin 13. 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 each device and thus requires individual calibration; therefore, the technique is unsuitable for mass production. The technique used in the ADT7467 is to measure the change in VBE when the device is operated at three currents. This is given by ΔVBE = kT/q × ln(N) where: k is Boltzmann’s constant. q is the charge on the carrier. T is the absolute temperature in Kelvin. N is the ratio of the two currents. Figure 23 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. It could also be a discrete transistor such as a 2N3904/2N3906. N2 × I IN1 × I IBIAS D+ D– LPF VDD VOUT+ VOUT– fC = 65kHz TO ADC REMOTE SENSING TRANSISTOR Figure 23. Signal Conditioning for Remote Diode Temperature Sensors 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 is connected to the D+ input. If an NPN transistor is used, the emitter is connected to the D− input and the base is connected to the D+ input. Figure 25 and Figure 26 show how to connect the ADT7467 to an NPN or PNP transistor for temperature measurement. To prevent ground noise from interfering with the measurement, 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 operating current through the sensor is switched among three related currents. Shown in Figure 23, N1 × I and N2 × I are different multiples of the current I. The currents through the temperature diode are switched between I and N1 × I, resulting in ΔVBE1; then they are switched between I and N2 × I, resulting in ΔVBE2. The temperature can then be calculated using the two ΔVBE measurements. This method can also cancel the effect of series resistance on the temperature measurement. The resulting ΔVBE waveforms are passed through a 65 kHz low-pass filter to remove noise and then sent to a chopper- stabilized amplifier that amplifies and rectifies the waveform to produce a dc voltage proportional to ΔVBE. The ADC digitizes this voltage, and a temperature measurement is produced. To reduce the effects of noise, digital filtering is performed by averaging the results of 16 measurement cycles. The results of remote temperature measurements are stored in 10-bit twos complement format, as listed in Table 7. The extra resolution for the temperature measurements is held in the Extended Resolution Register 2 (0x77). This produces tempera- ture readings with a resolution of 0.25°C. SERIES RESISTANCE CANCELLATION Parasitic resistance to the ADT7467 D+ and D− inputs (seen in series with the remote diode) is caused by a variety of factors, including PCB track resistance and track length. This series resistance appears as a temperature offset in the remote sensor’s temperature measurement. This error typically causes a 0.5°C off- set per 1 Ω of parasitic resistance in series with the remote diode. The ADT7467 automatically cancels the effect of this series resistance on the temperature reading, providing a more accurate result without the need for user characterization of this resistance. The ADT7467 is designed to automatically cancel, typically up to 3 kΩ of resistance. By using an advanced temperature measurement method, this is transparent to the user. This feature allows resistances to be added to the sensor path to produce a filter, allowing the part to be used in noisy environments. See the Noise Filtering section for details. Noise Filtering For temperature sensors operating in noisy environments, previous practice involved placing a capacitor across the D+ and D− pins to help combat the effects of noise. However, large capacitances affect the accuracy of the temperature measurement, leading to a recommended maximum capacitor value of 1000 pF. A capacitor of this value reduces the noise but does not eliminate it, making use of the sensor difficult in a very noisy environment. The ADT7467 has a major advantage over other devices for eliminating the effects of noise on the external sensor. Using the series resistance cancellation feature, a filter can be constructed between the external temperature sensor and the device. The effect of filter resistance seen in series with the remote sensor is automatically canceled from the temperature result. |
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