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TMP006B Datasheet(PDF) 25 Page - Texas Instruments |
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TMP006B Datasheet(HTML) 25 Page - Texas Instruments |
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25 / 38 page ![]() OBJ 30 nW T 140 mK 213 nW/K ' | 3 3 OUT 8 OBJ B OBJ det OBJ OBJ 3 0 V nW NEP T A 1 cos T 213 T R K H V T ' § · ' ' ¨ ¸ © ¹ . rms noise OBJ OUT Sensor 0.25 9 T 110 mK V 2 3 9. ' | ' . SENSOR OBJ ' V 2 3 T K K cos 3 3 8 OUT OBJ B OBJ det 0 OBJ 3 V T A 1 R T H V T ' ' . 2 2 2r cos 0 800 4r D T 4 4 3 SENSOR OBJ B OBJ DIE det 0 2 V = T T A (1 cos )R 3 H V T TMP006, TMP006B www.ti.com SBOS518E – MAY 2011 – REVISED APRIL 2015 Using the device-specific radiation transfer expression and R0, the detector response is shown in Equation 14: where • εOBJ is the emissivity of the object (0.95). • B is the Stefan-Boltzmann constant (5.67 × 10 -12 W/cm 2 /K 4). • TOBJ is the object temperature (273 K + 30°C). • TDIE is the detector temperature (273 K + 23°C). • Adet is the detector active area (1.09 × 10 -3 cm2) • θ is the half-angle subtended by the object as viewed from the detector. • R0 is the responsivity (~10.8 V/W for the specified temperatures). (14) The value of cos θ is shown in Equation 15: where • r is the distance between the detector and the object (10 mm). • D is the diameter of the object (15 mm). (15) Differentiating with respect to object temperature, a small change in temperature creates a small change in the measured voltage given by Equation 16: (16) Substituting values for the parameters yields Equation 17: (17) The sensor rms noise at TDIE = 25°C is ~0.25 µV; thus, the rms variation in temperature measurement is as shown in Equation 18: (18) The peak-to-peak noise is approximately six times the rms noise; therefore, estimate an accuracy of approximately ±0.33°C. This estimate can also be made using the noise-equivalent power (NEP), noting that NEP is the ratio of noise to responsivity, as shown in Equation 19: (19) Assuming the system is sensor-noise limited, the NEP is ~30 nW at 25°C, as shown in Equation 20: (20) Again, the peak-to-peak noise is approximately 6X the rms noise; therefore estimate an accuracy of approximately ±0.42°C. The different results from these two techniques is because of estimated values used for some parameters. The purpose of these techniques is not to obtain exact answers, but rather to quickly estimate the feasibility of a system implementation based on basic system parameters. These examples are intended only as guidelines; the specific values for the parameters depend on the specific system details. Copyright © 2011–2015, Texas Instruments Incorporated Submit Documentation Feedback 25 Product Folder Links: TMP006 TMP006B |
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