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MPXM2102AS Datasheet(PDF) 516 Page - Motorola, Inc |
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MPXM2102AS Datasheet(HTML) 516 Page - Motorola, Inc |
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516 / 670 page ![]() AN1586 3–370 Motorola Sensor Device Data www.motorola.com/semiconductors THE INTEGRATOR As shown in Figure 1. , the integrator consists of a single resistor and single capacitor. A programmable duty cycle pulse train from the microcontroller is input to the integrator. Assuming that the RC time constant of the integrator is sufficiently long compared to the pulse train’s frequency, the resulting output which is input to the inverting terminal of the comparator is a dc voltage that is linearly proportional to the pulse train’s duty cycle, i.e.: DC Output Voltage = Pulse Train’s Duty Cycle (%) • 5 V Where the Pulse Train’s Duty Cycle is multiplied by the pulse train’s logic–level one voltage value which is typically the same voltage as the microcontroller’s 5 V supply. Table 3 shows a few examples of Pulse Train Duty Cycles and the corresponding DC Output Voltage assuming a typical pulse train logic–level one value of 5 V. Table 3. Example Pulse Train Duty Cycles and the Integrator’s Corresponding dc Voltage Output Pulse Train’s Duty Cycle (%) 0 25 50 75 100 DC Output Voltage (V) 0 1.25 2.5 3.75 5 To establish a stable constant dc voltage at the integrator’s output, its time constant must be sufficiently long compared to the frequency of the pulse train. However, the system resolution and thus performance are directly related to the pulse train’s frequency. The design of the time constant and choice of the resistor and capacitor values is discussed in System Design: Defining and designing for a desired signal resolution. COMPARATOR The LM311 chip is designed specifically for use as a comparator and thus has short delay times, high slew rate, and an open–collector output. A pull–up resistor (R6 = 5 k Ω) at the output is all that is needed to obtain a rail–to–rail output. As Figure 1. shows, the pressure sensor’s amplified output voltage is input to the non–inverting terminal of the op amp and the integrator’s dc output voltage is input to the inverting terminal. Therefore, when the pressure sensor’s output voltage is greater than the integrator’s dc output voltage, the comparator’s output is high (logic–level one); conversely, when the pressure sensor’s output voltage is less than the integrator’s dc output voltage, the comparator’s output is low (logic–level zero). An optional resistor, RH is used as positive feedback around U2 in Figure 1 to provide a small amount of hysteresis to ensure a clean logic–level transition (prevents multiple transitions (squegging)) when the comparator’s inputs are similar in value. The amount of hysteresis increases as the value of RH decreases. For this design, the value of RH is not critical but should be on the order of 100 k Ω. THE MC68HC05P9 MICROCONTROLLER The microcontroller for this application requires an output compare timer channel and one general I/O pin. The output compare pin is programmed to output the pulse train that is input to the integrator, and the general I/O pin is configured as an input to monitor the logic–level of the comparator’s output. The remainder of this paper discusses the system and software requirements. SYSTEM DESIGN: HOW THE SYSTEM WORKS For any analog sensor voltage output, there’s a pulse train with a duty cycle that when integrated will equal the sensor’s output. Therefore, by incrementing via software the pulse train’s duty cycle from 0% to 100%, there’s a duty cycle that when integrated will be larger than the sensor’s current voltage output. When the integrated pulse train voltage becomes larger than the sensor’s output voltage, the comparator’s output will change from a logic–level one to a logic–level zero. This logic–level, in turn, is monitored on the general I/O pin. The pulse train’s duty cycle creating the integrated voltage that caused the comparator’s logic–level transition is the digital representation of the sensor’s voltage. Thus every sensor analog output voltage is mapped to a specific duty cycle. This design inherently has outstanding performance (very stable and accurate) since the digital representation of the sensor signal is created by the microcontroller’s digital time base. Also the pressure measurement, made via software that first increments the pulse train’s duty cycle and then determines if an edge transition occurred on the general I/O pin, is straightforward and easy. In a calibration routine (discussed below) the sensor’s output at two known pressures (e.g. zero and full–scale pressure) can be mapped to two corresponding pulse train duty cycles. Since the pressure sensor’s output voltage is linear with the applied pressure, and the integrator’s dc output voltage is linear with the input pulse train duty cycle, then the pulse train’s duty cycle that causes the logic–level transition at the comparator’s output will also be linear with the applied pressure. Thus by knowing the duty cycles for two known pressures, a linear interpolation of any duty cycle gives an accurate measurement of the current pressure. The following equation is used to interpolate the pressure measurement where the pressure units are in kPa: Duty Cycle @ Full–Scale Pressure – Duty Cycle @ Zero Pressure Current Duty Cycle – Duty Cycle @ Zero Pressure • Full–Scale Pressure in kPa Current Pressure = For example: At zero pressure, if the pulse train’s duty cycle required to cause a logic–level transition at the comparator’s output is 25% and at full–scale pressure the pulse train’s duty cycle is 75%, then the current pressure that corresponds to a duty cycle of 50% (required to obtain the logic–level one to logic–level zero transition at the comparator’s output) is Current Pressure + 50% – 25% 75% – 25% • 100 kPa = 50 kPa Until now, the pulse train has been defined in terms of duty cycle. However, in practice duty cycle is calculated from the ratio of the high time to the total period of the pulse train. Therefore, there is a high time (typically in µs) of the pulse train that causes the logic–level transition of the comparator’s output. The interpolation of the current pressure can then be calculated directly from the high time of the pulse train that is programmed by the user to be generated by the Freescale Semiconductor, Inc. For More Information On This Product, Go to: www.freescale.com |
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