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Micromachined thermal inclinometer based on flash evaporated Bi0.5Sb1.5Te3 (p)/Bi2Se0.3Te2.7(n) thermocouples

โœ Scribed by A. Giani; F. Mailly; M. Al khalfioui; A. Foucaran; A. Boyer


Publisher
Elsevier Science
Year
2004
Tongue
English
Weight
222 KB
Volume
107
Category
Article
ISSN
0921-5107

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โœฆ Synopsis


The techniques of micromachining are used for the manufacturing of a thermal inclinometer, which requires no solid proof mass and has a low-cost production. The sensor principle is as follows: a heating resistor creates a symmetrical temperature profile and two thermocouples, placed symmetrically on both sides of the heater, measure a differential temperature. When an acceleration is applied on the sensitive axis x of the sensor, the convection heat transfer and the temperature profile become asymmetric and the differential temperature was shown to be proportional to the acceleration and to the Grashof number. Platinum resistor deposited by electron beam evaporation and flash evaporated Bi 0.5 Sb 1.5 Te 3 (p)/Bi 2 Se 0.3 Te 2.7 (n) thermocouples are used, respectively, as heater and temperature sensors on a polyimide substrate. These ternary materials present higher figures of merit than 10 -3 K -1 and the thermocouple sensitivity is 440 V K -1 . Two types of sensors have been manufactured: the first one is deposited on a continuous polyimide film and the second one on a micromachined film, which permits to limit the energy consumption by a factor of 2 and to obtain a heater temperature rise of 3.44 K mW -1 and a sensitivity of 1410 V g -1 (1g = 9.81 m s -2 ) for a heating power of 100 mW.


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Improvement of thermal sensors based on
โœ A. Mzerd; F. Tcheliebou; A. Sackda; A. Boyer ๐Ÿ“‚ Article ๐Ÿ“… 1995 ๐Ÿ› Elsevier Science ๐ŸŒ English โš– 248 KB

Thermoelectric properties of materials are essentially based on the thermoelectrical figure of merit \(Z=S^{2} \sigma / K\), where \(S\) is the thermoelectrical power, \(\sigma\) the electrical conductivity and \(K\) the thermal conductivity. Narrow-bandgap semiconductors \(\mathrm{Bi}_{2} \mathrm{T