Pressure Transducer to ADC Application



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Application Report SLOA05 October 2000 Pressure Transducer to ADC Application John Bishop ABSTRACT Advanced Analog Products/OpAmp Applications A range of bridgetype transducers can measure numerous process variables. This report describes a pressure transducer, and a bridge transducer to measure strain in mechanical elements. It gives an example circuit from which to implement other applications. Introduction A major application of operational amplifiers (op amps) is converting and conditioning signals from transducers into signals that other devices such as analogtodigital converters (ADCs) can use. Conversion and conditioning are usually necessary because the transducer and ADC ranges and offsets are rarely the same. Op amp circuits are also useful in signal filtering for compatibility with ADC circuits. This report shows how to use a bridgetype transducer for measuring gas or liquid pressure and for measuring strain in mechanical elements, and pressure. A basic understanding of active and passive analog devices and their use is helpful to use this document to complete a design. Transducer Information The sensor tested in this application is a pressure transducer SX0 produced by SenSym. It is one of a set of solidstate pressure sensors with available fullscale ranges of 50 psi (7 kpa MPa). Three pressure measurement types are available: gauge, differential, and absolute. The device evaluated here has a fullscale pressure of psig (7 kpa). Its cost is low relative to other devices in this range; however, the low price is at the expense of no temperature compensation, a drawback that can be overcome by adding inexpensive, external, compensation components. SenSym defines three circuits for this purpose the method chosen here uses a NPN bipolar transistor and two resistors. Excitation Source Information For a bridge transducer to work it must be excited by a voltage source. Because the stability of the excitation voltage affects the accuracy of the measurement signal, a regulated voltage source is necessary. This application assumes the availability of a regulated 5V supply.

SLOA05 ADC Information For this design, Systems Engineering selected the TLV2544 ADC, which has an analog input range of 0 5 V(see http://www.ti.com/sc/docs/products/analog/tlv2544.html for its data sheet). Ideally, the span of the amplified sensor signal should fill this range. The voltage needed to power this device is a single 5V supply. Choice of Op Amp The ADC's 0 5 V analoginput range, and the fact that the power available was a single 5V supply required a railtorail output device. The op amp must also be able to handle the full input range of the transducer. For these reasons, the was chosen; its data sheet is at http://www.ti.com/sc/docs/products/analog/tlv2474.html Defining the Circuit The amplified pressure transducer signal is connected to an ADC. Since the ADC connects to a microprocessor or DSP, final calibrations can be done in software. Therefore, the 0 psi range should span the center of the range of the ADC. For calculating gain, the output range of the amplifier is 0 2.5 V. Figure is the schematic of the amplifier circuit for this application. 5V 5V C 3220 Ω 430 Ω U2 R8 R9 Q NPN 5V R3 00 nf 4 2 Ua 3 Vref BRIDGE Vin Vin2 R4 R5 C2 C 3320 Ω 500Ω Ub 5 7 R4 C3 R3a R3b C5 R 9 8 0 U2c R5 R2 R7 2 3 4 Ud R C7 Vout Figure. OpAmp Circuit for the Pressure Transducer to ADC Application 2 Pressure Transducer to ADC Application

SLOA05 The output of the circuit is: V OUT 2R R R R R 2R R R R R R = V 4 IN2 V R 3 R 7 R R 2 IN R 3 R REF R 5 R R 2 V () 3 5 7 2 3 2 5 7 2 When R 7 =R, R 5 =R 2, and R 4 =R, equation () reduces to: 2R R V OUT = (V IN 2 VIN ) VREF R 3 R (2) 2 Solving for R 3 gives: ( VOUT VREF ) R2 R3 = 2R (3) ( VIN 2 VIN) R The sensitivity of the bridge is typically 4.0 mv/v/psi. The pressure range is psi and the excitation voltage is 5 V. Therefore, the differential output of the sensor (V IN2 V IN )from0topsi is 20 mv. Setting R =R 4 =R =R 7 = 20.0 kω (% value), and R 2 =R 5 =2.0kΩ results in a fullscale output of 2.5 V when R 3 = 3.478 kω. A unique feature of this precision instrumentation amplifier is the ability to control the total gain of the amplifier with one resistor. Calibration Devices The resistor that controls gain is R. A potentiometer has a larger temperature coefficient and is more likely to drift over time than a fixed resistor. Placing a fixed resistor in series with a potentiometer reduces this. The values calculated in the following equations are based on about 0% gain adjustment: R 3A = R R (5%) = 43 kω (% resistor) (4) R 3B = R 3 (0%) = 50 kω (Cermet potentiometer) (5) The potentiometer for adjusting offset, R3 is not critical but a 0kΩ multiturn potentiometer uses 0.5 ma. One of the goals of design is to reduce components without compromising function. If the offset voltage of the op amps is low enough, replacing potentiometers with fixed resistors is possible. Offset and gain calibration would then be done using software in a DSP or microprocessor. This is possible because the bottom and top 25% of the input range of the ADC are not presently used. In this condition, V REF would be initially set by replacing R3 with a voltage divider. The offset drift of the op amps cause the output to move up or down into the unused areas. Variations on the resistors cause small gain errors but these should be of less concern than the offset voltage. Instead of calibrating with potentiometers, using the offset and gain variables in calculations can generate a calibrated output. Pressure Transducer to ADC Application 3

SLOA05 Signal Filtering If the transducer is installed on the amplifier board, the input filter circuits and shielded wires are not needed. Connecting a transducer to an input, subjects the wiring to noise signals because of the surrounding electrical and magnetic environment. To prevent this noise from interfering with the measurement signals, some shielding is necessary. Using a twisted pair from the transducer to the conversion circuit and shielding this pair (grounding the shield at the instrument) reduces the noise. Even when the transducer is connected through correctlyshielded cabling, some noise is brought into the amplifier along with the measurement signal. Without an input filter, the op amp would act as an RF detector, converting highfrequency signals from other devices into signals with lowfrequency components. Placing a resistor and capacitor on the input forms a lowpass filter and prevents radiofrequency signals from interfering with the measurement signal. The frequency response of this filter is: F C = 2πRC (5) Thus, if R 4 and R 5 are0kω, and C 2 and C are0nf,thenf C is about 00 Hz. The next two stages have capacitors in parallel with the feedback resistors. The frequency response of these filters is also defined by equation (5). Using for the feedback resistor gives a cutoff frequency, F C, of about 800 Hz. Bibliography For more information, you can access the following reports as.pdf files at http://www.ti.com/ by searching for the literature numbers indicated.. Understanding Basic Analog Ideal Op Amps, Texas Instruments Literature Number SLAA08. 2. Single Supply Operational Amplifier Design Techniques, Texas Instruments Literature Number SLOA030. 3. Active Low Pass Filter Design, Texas Instruments Literature Number SLOA049. 4. Use Of RailToRail Operational Amplifiers, Texas Instruments Literature Number SLOA039 (Revision A). 5. Sensor to ADCAnalog Interface Design, Texas Instruments Literature Number SLYT05 (page 22). MixedSignal: Amplifiers: Operational Amplifiers (This is a complete op amp application index). http://www.ti.com/sc/docs/apps/analog/operational_amplifiers.html 7. Signal Conditioning Wheatstone Resistive Bridge Sensors, Texas Instruments Literature Number SLOA034. 4 Pressure Transducer to ADC Application

SLOA05 Appendix A. Calculations The following spreadsheet output indicates values and equations used in this application note. 5V 5V C 3220 Ω 430 Ω R8 R9 Q NPN 5V R3 00 nf 4 2 Ua 3 Vref U2 BRIDGE Vin2 R4 Vin R5 C2 C 3320 Ω 500Ω Ub 5 7 R4 C3 R3a R3b C5 R 9 0 8 U2c R5 R2 R7 2 4 3 Ud Vout R C7 Given: OUTPUTmin= 0.0 psi OUTPUTmin= 0 V INPUTmax=.0 psi OUTPUTmax= 2.5 V Sensitivity 0.004 mv/v/psi Exitation Voltage 5 V Full Scale Span 0.02 V R 8 = 3.22k Ohms Nominal Gain 25 R 9 =.43k Ohms R = R4 = R7 = R= 20000 Ohms R5 = R2 = 2000 Ohms Vin= 0.02 V vout= 2.5 V R3= 3478 Ohms % value R3A= 3304 3320 Ohms Pot. Value R3B= 348 500 Ohms C 4 =C = 0.0 uf C 3 =C 5 =C 7 = 0.0 uf R 4 =R 5 = 0000 Ohms R =R 4 =R = 20000 Ohms F C = 592 Hz F C = 79 Hz Note: Values in solid boxes are entered values while values in dashed boxes are calculated. Pressure Transducer to ADC Application 5

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