SX01DD4

SX15A SENSORTECHNICS | Alldatasheet

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Technical content

www.sensortechnics.com SXxxxGD2 DIP SXxxxAD2 SXxxxD4 DIP Button sensor or "N" package Output Vs Vs Output

FEATURES

• Absolute, differential and gage devices
• High impedance bridge
• Low power consumption for battery operation

APPLICATIONS

• Industrial controls
• Pneumatic controls
• Medical instrumentation
• Barometry GENERAL DESCRIPTION The SX series of pressure sensors provides the most cost effective method of measuring pressures up to 150 psi. These sensors were specifically designed to be used with non-corrosive and non-ionic media, such as air and dry gases. Convenient pressure ranges are available to measure differential, gage and absolute pressures from 0 to 1 psi up to 0 to 150 psi. The absolute (A) devices have an in- ternal vacuum reference and an output voltage proportional to absolute pressure. The differential (D) devices allow application of pressure to either side of the diaphragm and can be used for gage or differential pressure measurements. This product is packaged either in SenSym's standard low cost chip carrier "button" package, a plastic ported "N" package or a dual inline package (DIP). All packages are designed for applications where the sensing element is to be integral to the OEM equipment. These packages can be o-ring sealed, epoxied, and/or clamped onto a pressure fitting. A closed bridge 4-pin SIP configuration is provided for electrical connection to the button or "N" package. Because of its high-impedance bridge, the SX series is ideal for portable and low power or battery opera-ted systems. Due to its low noise, the SX is an excellent choice for medical and low pressure measurements. The polarity indicated is for pressure applied to: SX... : P1 (forward gage) SX...AD2 : P1 (forward gage) SX...GD2 : P2 (backward gage) SX...DD4 : P2 (backward gage) ELECTRICAL CONNECTION Button sensor +VS 3 out -4 1GND out +2 P1 DIP package EQUIVALENT CIRCUIT P1GND +Vs 4 vent hole out - 4out + +Vs out - +Vs 1P2 out + GND

1 P1out -

+Vs 1out + 4 +VsP2 +Vs

www.sensortechnics.com Maximum ratings Suppy voltage, VS +12 VDC Temperature ranges Operating -40°C to +85°C Storage -55°C to +125°C Maximum pressure at any port11 150 psig Lead temperature (soldering 4 sec.) 250 °C scitsiretcarahC. niM. pyT. xaMt inU tesffoerusserporeZ 9 53-0 2-0 V m stceffeerutarepmeTt esffO4 ±C °/V/Vµ )C°07ot0( 7,4 napS0 552-0 512-0 091- C°/mppecnadepmiegdirB0 96+0 57+0 18+ siseretsyhdnaytiraenildenibmoC 2 2.0±5 .0± SSF%ytilibataepeR 3 5.0± napsdnatesffofoytilibatsmretgnoL 6 1.0±V m ecnadepmitupnI 1.4 kΩecnadepmituptuO 1.4 emitesnopseR 5 1.0s m PERFORMANCE CHARACTERISTICS (Vs = 5.0 ± 0.01 V, tamb = 25 °C, common-mode pressure = 0 psig, pressure applied to P1 for Button, N and A2 housings, pressure applied to P2 for G2 and D4 housings) PRESSURE SENSOR CHARACTERISTICS (Vs = 5.0 ± 0.01 V, tamb = 25 °C, common-mode pressure = 0 psig, pressure applied to P1 for Button, N and A2 housings, pressure applied to P2 for G2 and D4 housings) rebmuntraPe russerpgnitarepOe russerpfoorP 8 napselacs-lluF 1 .niM. pyT. xaM

www.sensortechnics.com TYPICAL PERFORMANCE CHARACTERISTICS Specification notes: Span is the algebraic difference between the output voltage at full-scale pressure and the output at zero pressure. Hysteresis is the maximum output difference at any point within the operating pressure range for increasing and decreasing pressure. Linearity is the maximum deviation of measure output at constant temperature (25°C) from "Best Straight Line" determined by three points, offset, full scale pressure and half full scale pressure. Maximum difference in output at any pressure with the operating pressure range and temperature within 0°C to +70°C after: a) 100 temperature cycles, 0°C to +70°C b) 1.0 million pressure cycles, 0 psi to full scale span Slope of the best straight line from 0°C and 70°C. For operation outside this temperature, contact Sensortechnics for more specific applications information. Response time for a 0 to full-scale span pressure step change. Long term stability over a one year period . This parameter is not 100 % tested. It is guaranteed by process design and tested on a sample basis only. If the proof pressure is exceeded, even momentarily, the package may leak or burst, or the pressure sensing die may fracture. Note: The proof pressure for the forward gage of all devices in the D4-package is the specified value or 100 psi, whatever is less.

www.sensortechnics.com MECHANICAL AND MOUNTING CONSIDERATIONS PHYSICAL CONSTRUCTION Button sensor element The button sensor element was designed to allow easy interface with additional cases and housings which then allow pressure connection. The device can be mounted with an o-ring, gasket, or RTV seals on one or both sides of the device. The device can then be glued or clamped into a variety of fixtures and the leads can be bent as necessary to allow for ease of electrical connection. However, caution is advised as repeated bending of the leads will cause eventual breakage. For most gage applications, pressure should be applied to the top side of the device (see Physical Construction Drawing). For differential applications, the top side of the device (P1) should be used as the high pressure port and the bottom (P2) as the low pressure port. The button SX package has a very small internal volume of 0.06 cubic centimeters for P1 and 0.001 cubic centimeters for P2. “N” packaged sensor The "N” packaged sensor is designed for convenient pressure connection and easy PC board mounting. To mount the device horizontally to a PC board, the leads can be bent downward and the package attached to the board using either tie wraps or mounting screws. For pressure attachment, tygon or silicon tubing is recommended. The “N” package version of the sensor has two (2) tubes available for pressure connec-tion. For gage devices, pressure should be applied to port P1. For differential pressure applications, port P1 should be used as the high pressure port and P2 should be used as the low pressure port. GENERAL DISCUSSION Output characteristics The SX series devices give a voltage output which is directly proportional to applied pressure. The devices will give an increase in positive going output when increasing pressure is applied to pressure port P1 of the device. If the devices are operated in the backward gage mode, the output will increase with decreases in pressure. The devices are ratiometric to the supply voltage. Changes in supply voltage will cause proportional changes in the offset voltage and full-scale span. User calibration SX series devices feature the button IC pressure sensor element. This will keep overall system costs down by allowing the user to select calibration and temperature compensation circuits which specifically match individual application needs. In most cases, the primary signal conditioning elements to be added to the SX by the user are: offset and span calibration and temperature compensation. Some typical circuits are shown in the application section. Vacuum reference (absolute devices) Absolute sensors have a hermetically sealed vacuum reference chamber. The offset voltage on these units is therefore measured at vacuum, 0 psia. Since all pressure is measured relative to a vacuum reference, all changes in barometric pressure or changes in altitude will cause changes in the device output. Media compatibility SX devices are compatible with most non- corrosive gases. Because the circuitry is coated with a protective silicon gel, some otherwise corrosive environments can be compatible with the sensors. As shown in the physical construction diagram below for the button sensor element and ,,N” package, fluids must generally be compatible with silicon gel, RTV, plastic, and aluminum for forward gage use and RTV, silicon, glass and aluminum for backward gage or differential applications. For questions concerning media compatibility, contact the factory.

www.sensortechnics.com General The SX family of pressure sensors functions as a Wheatstone bridge. When pressure is applied to the device (see Figure I) the resistors in the arms of the bridge change by an amount ∆. Figure I. Button sensor bridge schematic The resulting differential output voltage V0 is easily shown to be VO = VB x ∆. Since the change in resistance is directly pro- portional to pressure, VO can be written as: VO = S x P x VB ± VOS (1) Where: VO is the output voltage in mV S is the sensitivity in mV/V per psi P is the pressure in psi VB is the bridge voltage in volts. VOS is the offset error (the differential output voltage when the applied pressure is zero). The offset voltage presents little problem in most applications, since it can easily be corrected for in the amplifier circuitry, or corrected digitally if a microprocessor is used in the system. Temperature effects In this discussion, for simplicity of notation, the change of a variable with temperature will be designated with a dot () over the variable. For example, change in sensitivity δS change in temperature δT From equation (1), and ignoring the VOS term, it in seen that for a given constant pressure, the output voltage change, as a function of temperature*, is: VO = SPVB (2) Thus, in order for output voltage to be inde- pendent of temperature, the voltage across the bridge, VB, must change with tempera- ture in the "opposite direction” from the sensitivity change with temperature. From the typical curves for the temperature dependence of span (span = S x P x VB),

APPLICATION INFORMATION

S == it can be seen that the sensitivity change with temperature is slightly non-linear and can be correlated very well with an equation of the form: S = SO [(1 - ßTD ) + ρTD 2] (3) where TD is the temperature difference between 25°C and the temperature of inte- rest, SO is the sensitivity at 25°C, and beta (ß) and rho (ρ) are correlation constants. Fortunately, between 0°C and 70°C the change in sensitivity with temperature is quite linear, and excellent results can be obtained over this temperature range by ignoring the second-order temperature dependent term. Operating outside the 0°C and 70°C temperature range will require a more rigorous mathematical approach and the use of non-linear compensating cir- cuitry, if accuracy of better than ±1 % is re- quired. Because the majority of SX appli- cations fall within the 0°C to 70°C operating temperature range, the discussion and circuit designs given here will ignore the non-linear effects. Thus: S = SO (1 - ßTD ) (4) Substituting equation (4) into equation (1) and ignoring VOS , it can be shown that the necessary bridge voltage, VB, will be of the form: VBO (1-ßTD) where VBO is the bridge voltage at 25°C. This equation is again non-linear. However, for the temperature range of interest, and since ß is small (0.215%/°C from the electrical tables), the above expression can be approximated by: VB=V BO [1 +ßTD ] with less than 1 % error. Thus to compen- sate for a negative 2150 ppm/°C sensitivity change with temperature, the bridge voltage should increase with temperature at a rate of +2150 ppm/°C. The above value of bridge voltage change will be used in the circuit discussions that follow. That is to say, the required change in terms of ppm/°C is: = +2050 ppm/°C The bridge input resistance*, RB also changes with temperature and is quite linear in the temperature range of interest. The bridge resistance has a temperature coefficient of typically: = +750 ppm/°C VB= =V BO [(1 - ßTD + (ßTD )2+...)] This term enters into several compensation circuit equations, particularly when the bridge excitation is from a constant current source. To summarize, the following list indicates how the sensor variables can be accommo- dated  Full-scale span from device to device. Make the gain adjustment in the op amp circuitry  Temperature coefficient of span: 1) temperature compensate the bridge or 2) temperature compensate the op amp gain  Offset voltage: Adjustment in op amp circuitry  Offset voltage temperature coefficient: Usually can be ignored. For more precise design requirements, contact the factory for information on how to compensate for this term. Bridge compensation circuits Although thermistors can be used to tempe- rature compensate the bridge (and in fact will be required for extended temperature operation), they are inherently non-linear, difficult to use in volume production, and more expensive than the circuit approaches shown here, which use inexpensive semi- conductor devices The circuits shown have been designed to incorporate a minimum number of adjustments and allow inter- changeability of devices with little variation from device to device. In general, equations for the bridge voltage and its change with temperature are given to enable the user to modify or adjust the circuitry as required. 1. Diode string (Figure II) For systems using 6 V supplies, this method of compensating for the effects of span over temperature is the lowest cost solution The diodes are small signal silicon diodes, such as 1N914 or 1N4148, and do not have to be matched. Figure II. Diode String Span Compensation VB VB ( ) R B R B( )

www.sensortechnics.com ( )[ ( )] IO RB IO R B( ) a) V B = α (VS + IO R 2)   b) = (1 - α)+ 1-α c) α =   d) = 3360 ppm/°C, =+750ppm/°C e) I O= The design steps are straight forward: 1) Knowing VS and the desired bridge voltage VB, solve equation (b) for α. 2) Now, solve equation (c) for R2, letting RB = 4650Ω. 3) Solve equation (a) for IO . 4) Find R1 or its nearest 1% tolerance value from equation (e). Table II gives specific 1% resistor values in ohms, for several popular system voltages. For best results, the resistors should be 1% metal film with a low temperature coefficient. Table II. Selected R values vs VS for figure IV VS VB R 1(Ω)R 2(Ω) 5V 3V 147 11.0k 6V 4V 105 9.53k 9V 6V 68.1 9.53k 12V 9V 43.2 8.25k 15V 10V 41.2 9.53k Amplifier design There are hundreds of instrumentation amplifier designs, and the intent here will be to briefly describe one circuit which:

• does not load the bridge
• involves minimal components
• provides excellent performance Amplifier adjustment procedure 1. Without pressure applied, (a) Short points A and B together as shown in Figure V. Adjust the 1 k c o m m o n - m o d e r e j e c t i o n (CMRR) pot until the voltage at test point (Tp) Vx is equal to the voltage at test point (Tp) VR . This is easily accomplished by placing a digital voltmeter between these test points and adjusting for 0.000. VB R B IO VS VB R B IO VB( )( ) 67.7 mV R 1 R B R 2 + RB ( ) a) V B=V S-4φ b) V B VB VS φ c) = -2500 ppm/°C for silicon diodes Figure II. Equations For example, solving equation (b) for VB/ VB when VS = 6.0 V φ = 0.7 V Yields: = 2188 ppm/°C Since the sensor’s span changes with tem- perature at -2150 ppm/°C, this technique will typically result in an overall negative TC of 38 ppm/C. This error is acceptable in most applications. For operation with VS above 6V, it is recom- mended to use the transistor or constant current compensation technique. 2. Transistor compensation network Figure III uses a single transistor to simulate a diode string, with the equations as shown. The values shown in Table I were found to give excellent results over 0°C to 70°C. Again, if precision temperature compen- sation is required for each device, the fixed value resistors shown for R1 in Table I can be replaced by a 3.24k resistor in series with a 1k pot. Then, each devices temperature compensation can be individually adjusted. Figure III. Transistor/Resistor span TC compensation ( )( )( ) φ φ( ) φ φ VB VB a) VB = VS - α φ b) = - x - α c) α =1+ d) φ φ Table I. Selected R values vs VS for figure III VS R 1 (Ω)R 2 (Ω) 5V 3.32k 1.43k 9V 4.02k 806 12V 4.22k 604 3. Constant current excitation (Figure IV) The circuits shown in Figures II and III, although simple and inexpensive, have one drawback in that the voltage across the bridge is determined by the compensation network. That is, the compensation network is determined and what voltage is “leftover" is across the bridge. The circuit of Figure IV solves this problem and allows the bridge voltage to be independently selected. In Figure IV, the bridge is driven from a constant current source, the LM334, which has a very well known and repeatable temperature coefficient of +3300 ppm/°C. This temperature coefficient (TC), in conjunction with the TC of the bridge resis- tance, is too high to compensate the sensitivity TC, hence resistor R2 is added to reduce the total circuit TC. The basic design steps for this method of temperature compensation are shown below. However, please refer to SenSym’s Application Note SSAN-16 for details on the temperature compensation technique. Figure IV. Constant current span TC Compensation ( ) ( )( ) VB φα VB φ VS φ R 1 R 2 = -2500 ppm/°C( ) APPLICATION INFORMATION (cont.)

www.sensortechnics.com Table III. For 0 to 70°C operation SPAN VS VB R 2 R 1 FS R 5 R p 5V 3.5V 9.09k 118 Ω 3V 604 Ω 2k 6V 4.5V 8.45k 86.6 Ω 4V 604 Ω 2k 9V 7V 7.87k 54.9 Ω 5V 1k 2k 12V 10V 7.15k 36.5 Ω 5V 1.82k 5k 12V 10V 7.15k 36.5 Ω 10V 511 Ω 2k 15V 12V 7.68k 31.6 Ω 5V 1.4k 5k 15V 12V 8.87k 31.6 Ω 10V 604 Ω 2k APPLICATION INFORMATION (cont.) (b) Remove the short and adjust the 500 Ω offset adjust pot until Vx is again equal to VR . (c) Adjust the 2k reference (VR ) adjust pot to get an output voltage (VO ) equal to 1.00V. 2. Apply the fuII-scale pressure and adjust the span adjust pot, R5, to get the output voltage that is desired to represent full- scale. Note: Application information shown here is based on the closed bridge configuration. The choice of the operational amplifiers to use is based on individual cost/performance trade-offs. The accuracy will be primarily limited by the amplifier’s common-mode rejection, offset voltage drift with tempera- ture and noise performance. Low cost, low performance devices, such as the LM324 can be used if the temperature ranges limited to 25°C +15°C and an accuracy of +2% is adequate. For more precise applications amplifiers such as the LT1014 and LT1002 have been found to be excellent. An amplifier that uses a single supply is shown in Figure V. Table III gives resistor values for various supply and full-scale output combinations. Factory compensated devices This application note provides the neces- sary information for temperature compen- sating and calibrating the SX sensors. In some case, the customer may find that SX devices which have been factory adjusted for temperature compensation and span are more economical for a particular application. SenSym does offer devices with this feature. For more information on these factory calibrated and compensated devices, the SCX series and SDX series, please contact Sensortechnics. Figure V: Button Sensor Amplifier Circuit A = LT1014CN V O = 4 [1 + ] VIN + VR B = LM10CN Resistors labled R3 are 5-Element Resistor Arrays 10 kΩ. Two required 10k RG

www.sensortechnics.com PHYSICAL DIMENSIONS Button package N package mass: 1 g dimensions in inches (mm) mass: 5 g dimensions in inches (mm)

www.sensortechnics.com PHYSICAL DIMENSIONS Basic sensor DIP "D2" package Basic sensor DIP "D4" package mass: 1 g dimensions in inches (mm) mass: 1 g dimensions in inches (mm) 0.020 typ. (0.51) 0.110 typ. (2.79) 0.380 (9.65) 0.285 (7.24) 0.090 typ. (2.29) 0.470 (11.94)0.050 typ. (1.27) 0.550 (13.97) 0.600 (15.24) 0.01 (0.25) 0.100 typ. (2.54) 0.300 (7.62) 0.070 (1.78) 0.135 (3.43) 0.250 (6.35)

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ORDERING INFORMATION

SenSym and Sensortechnics reserve the right to make changes to any products herein. SenSym and Sensortechnics do not assume any liability arising out of the application or use of any product or circuit described herein, neither does it convey any license under its patent rights nor the rights of others. egnarerusserP .ontrapredrO egakcapnottuBe gakcap"N" egakcap"2D"PID )detropelgnis( egakcap"4D"PID )detroplaud( etulosbA erusserp isp51-0A 51XSN A51XS2 DA51XS- -- isp03-0A 03XSN A03XS2 DA03XS- -- isp001-0A 001XSN A001XS2 DA001XS- -- egaG erusserp isp1-0 esu laitnereffid secived esu laitnereffid secived 2DG10XS- -- isp5-02 DG50XS- -- isp51-02 DG51XS- -- isp03-02 DG03XS- -- isp001-02 DG001XS- -- isp051-0- --- -- laitnereffiD erusserp isp1-0D 10XSN D10XS- --4 DD10XS isp5-0D 50XSN D50XS- --4 DD50XS isp51-0D 51XSN D51XS- --4 DD51XS isp03-0D 03XSN D03XS- --4 DD03XS isp001-0D 001XSN D001XS- --4 DD001XS isp051-0D 051XSN D051XS- --- --