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MPXM2102AS 数据表(PDF) 338 Page - Motorola, Inc |
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MPXM2102AS 数据表(HTML) 338 Page - Motorola, Inc |
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338 / 670 page ![]() AN935 3–192 Motorola Sensor Device Data www.motorola.com/semiconductors A second technique that still uses a single pressure measurement as the input was investigated. In this method, the sensitivity coefficients are calculated using a piece–wise linearization technique where the total span variation is divided into four windows of 10 mV (i.e., 30–39.99, 40–49.99, etc.) and coefficients calculated for each window. The errors that arise out of using this method are shown in Figures 10 through 13. This method results in a large majority of the devices having errors <0.5%, while only one of the devices was >1%. The sensitivity coefficients that are substituted into equation [2] for the different techniques are given in Table 1. It is important to note that for either technique the only measurement that is required by the user in order to clearly determine the sensitivity coefficients is the determination of the full scale span of the particular pressure transducer. Figure 10. Linearity Error of Piece–Wise Linear Fit at 1/4 FS 48 42 36 30 24 18 12 6.0 0.0 37.69 33.92 30.15 26.38 22.62 18.85 15.08 11.31 7.54 3.77 – 2.0 –1.6 –1.4 –1.2 –1.0 – 0.8 – 0.6 – 0.4 – 0.2 0.0 0.2 0.4 0.6 0.8 1.0 1.2 1.4 1.6 1.8 2.0 NO. OF UNITS LINEARITY ERROR (% FS) General Fit P = 1/4 FS Average Error = 0.18 Standard Deviation = 0.159 % –1.8 Table 1. Comparison of Linearization Methods SPAN WINDOW B0 B1 B2 GENERAL FIT 0.1045 + 2.95E – 3X 0.2055 + 1.598E – 3X + 1.723E – 4X2 1.293E – 13X5.681 PIECE–WISE LINEAR FIT 30–39.99 0.08209 – 2.246E – 3X 0.02433 = 1.430E – 2X –1.961E – 4 + 8.816E – 6X 40–49.99 0.1803 – 4.67E – 3X –0.119 + 1.655E – 2X –1.572E – 3 + 4.247E – 5X 50–59.99 0.1055 – 3.051E – 3X –0.355 + 2.126E – 2X –5.0813 – 3 + 1.116E – 4X 60–69.99 –0.288 + 3.473E – 3X –0.361 + 2.145E – 2X –5.928E – 3 + 1.259E – 4X X = Full Scale Span Freescale Semiconductor, Inc. For More Information On This Product, Go to: www.freescale.com |
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