TB3016 Using the PIC® MCU CTMU for Temperature Measurement Author: Padmaraja Yedamale Microchip Technology Inc. The Charge Time Measurement Unit (CTMU), introduced on the latest generation of PIC24F and PIC18F devices, uses a constant current source to calculate both capacitance changes and the time difference between events. The same current source can also be used to measure temperature by exploiting a basic principle of semiconductor physics. This allows the use of a common and inexpensive diode, in the place of a relatively more expensive thermistor or other temperature sensor. This brief describes the basic concepts of temperature measurement using the CTMU. IMPLEMENTATION To implement this theory, all that is needed is to connect a regular junction diode to one of the microcontroller’s A/D pins (Figure 1). The A/D channel multiplexer is shared by the CTMU and the ADC. To perform a measurement, the multiplexer is configured to select the pin connected to the diode. The CTMU current source is then turned on, and an A/D conversion is performed on the channel. As shown in the equivalent circuit diagram, the diode is driven by the CTMU at IF. The resulting VF across the diode is measured by the ADC. FIGURE 1: CTMU TEMPERATURE MEASUREMENT CIRCUIT BASIC PRINCIPLE We can show that the forward voltage (VF) of a P-N junction, such as a diode, is an extension of the equation for the junction’s thermal voltage: Simplified Block Diagram PIC® microcontroller Current Source I kT V F = ------ ln ⎛ 1 – ----F-⎞ ⎝ q IS ⎠ where k is the Boltzmann constant (1.38 x 10-23 J K-1), T is the absolute junction temperature in kelvin, q is the electron charge (1.6 x 10-19 C), IF is the forward current applied to the diode, and IS is the diode’s characteristic saturation current. Since k and q are physical constants, and IS is a constant for the device, this only leaves T and IF as independent variables. If IF is held constant, it follows from the equation that VF will vary as a function of T. As the natural log term of the equation will always be negative, the temperature will be negatively proportional to VF. In other words, as temperature increases, VF decreases. CTMU A/D Converter ANx A/D MUX VF Equivalent Circuit By using the CTMU’s current source to provide a constant IF, it becomes possible to calculate the temperature by measuring the VF across the diode. CTMU ADC IF VF © 2009 Microchip Technology Inc. DS93016A-page 1 TB3016 EXPERIMENTAL VALIDATION Resolution (expressed as temperature per ADC counts) is calculated as: To test the theory, several devices with simple P-N junctions were tested in a controlled temperature environment while measuring VF as previously described. Included in the testing were three common silicon diodes, two common bipolar transistors, and two LEDs. An additional trial was run with two diodes (1N914) connected in parallel as a single unit. Each device was evaluated using an ADC voltage reference (VREF) of 3.3V. Temperature was varied from 0°C to 105°C inclusive, with 256 conversions being taken at roughly 5°C intervals over this range. The ADC readings (proportional to voltage) were recorded for each temperature point. These readings were used to directly calculate resolution, and converted to voltage to calculate line slope. TABLE 1: Number of samples × Temperature range -------------------------------------------------------------------------------------------------------------------------------------Counts at min temperature – Counts at max tempertaure The results of the trial are summarized in Table 1, and presented in graphic form in Figure 2. As can be seen, the correlation between temperature and VF is negative. Also as expected, the relationship between temperature and the forward voltage on the junction is essentially linear. This makes it possible for any readily available diode – or for that matter, any inexpensive semiconductor – to function as a low-resolution temperature sensor in conjunction with the CTMU. EXPERIMENTAL VF VALUES (AS ADC COUNTS) FOR DIFFERENT DEVICES AS A FUNCTION OF TEMPERATURE ADC Readings (256 samples) Min. Temp Max. Temp Resolution (°C/Count) 1N4007 36,890 12,815 1.12 1N4148 32,500 8,980 1.15 -2.8 mV/°C 1N914 31,500 6,417 1.08 -2.98 mV/°C 2N3904 (NPN) 45,100 23,560 1.26 -2.56 mV/°C 2N3906 (PNP) 43,860 22,020 1.24 -2.60 mV/°C SML-LXT0805GW-TR (Green LED) 52,500 27,150 1.07 -3.01 mV/°C CML 5311F (Red LED) 54,280 32,265 1.23 -2.62 mV/°C Two 1N914 (parallel) 31,500 6,660 1.09 -2.95 mV/°C Component DS93016A-page 2 Slope -2.88 mV/°C © 2009 Microchip Technology Inc. TB3016 FIGURE 2: ADC VALUES AS A FUNCTION OF TEMPERATURE FOR TESTED DEVICES 60000 1N4007 1N4148 1N914 50000 LED-D22 2N3904(NPN) ADC count (x256) LED-D27 40000 2N3906(PNP) 2|| 1N914 30000 20000 10000 0 0 20 40 60 80 100 120 Temperature (C) INCREASING TEMPERATURE MEASUREMENT RESOLUTION The method described here is adequate for resolution of about 1°C. In most cases, this represents an A/D channel voltage change of about 3 mV. At this scale, attempts to get better resolution will run into the limitations of the A/D converter. To achieve higher temperature resolutions, some minor changes to the conversion method are needed. These include: • Using a lower reference voltage for the ADC. One significant determining factor in temperature resolution is the selection of VREF. Smaller values of VREF tend to produce a larger difference voltage to be converted; this produces a larger incremental reading per degree, and thus higher resolution. Table 2 shows the expected temperature resolution for the same experiment, assuming an ADC VREF of 2.0V. • Using two diodes in series. Although this does not increase resolution per se, the resulting doubling of the change in the measured voltage per unit of temperature will result in increased accuracy. • Adding a single stage of voltage amplification with an op amp. By increasing the voltage to the ADC and matching it to the ADC voltage reference, resolution is increased. Although this adds several external components and some cost to the solution, this may be desirable in applications where a more precise determination of temperature is required. © 2009 Microchip Technology Inc. TABLE 2: EXPECTED TEMPERATURE RESOLUTION FOR VREF OF 2.0V Resolution (°C/Count) Component VREF = 3.3V (observed) VREF = 2.0V (predicted) 1N4007 1.12 0.68 1N4148 1.15 0.69 1N914 1.08 0.66 2N3904 1.26 0.76 2N3906 1.24 0.75 SML-LXT0805GW-TR 1.07 0.64 CML 5311F 1.23 0.74 Two 1N914 (parallel) 1.09 0.66 DS93016A-page 3 TB3016 CONCLUSION For applications using a PIC18F or PIC24F microcontroller with the CTMU, adding a temperature function does not depend on the use of a special temperature sensor; it can be done using a commodity diode and a small addition of code to the application firmware. This makes the incremental cost of adding the additional feature very small indeed. REFERENCES PIC24F Family Reference Manual, Section 11, “Charge Time Measurement Unit (CTMU)” (DS39724). Microchip Technology Inc., 2008. DS93016A-page 4 © 2009 Microchip Technology Inc. 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Analog-for-the-Digital Age, Application Maestro, CodeGuard, dsPICDEM, dsPICDEM.net, dsPICworks, dsSPEAK, ECAN, ECONOMONITOR, FanSense, In-Circuit Serial Programming, ICSP, ICEPIC, Mindi, MiWi, MPASM, MPLAB Certified logo, MPLIB, MPLINK, mTouch, PICkit, PICDEM, PICDEM.net, PICtail, PIC32 logo, PowerCal, PowerInfo, PowerMate, PowerTool, REAL ICE, rfLAB, Select Mode, Total Endurance, WiperLock and ZENA are trademarks of Microchip Technology Incorporated in the U.S.A. and other countries. SQTP is a service mark of Microchip Technology Incorporated in the U.S.A. All other trademarks mentioned herein are property of their respective companies. © 2009, Microchip Technology Incorporated, Printed in the U.S.A., All Rights Reserved. Printed on recycled paper. Microchip received ISO/TS-16949:2002 certification for its worldwide headquarters, design and wafer fabrication facilities in Chandler and Tempe, Arizona; Gresham, Oregon and design centers in California and India. 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