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Journal articles on the topic 'Calorimetric sensor'

Author: Grafiati

Published: 4 June 2021

Last updated: 5 February 2022

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1

Ghouila-Houri, Cécile, Célestin Ott, Romain Viard, Quentin Gallas, Eric Garnier, Abdelkrim Talbi, and Philippe Pernod. "Robust Calorimetric Micro-Sensor for Aerodynamic Applications." Proceedings 2, no. 13 (November 27, 2018): 794. http://dx.doi.org/10.3390/proceedings2130794.

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This paper reports a calorimetric micro-sensor designed for aerodynamic applications. Measuring both the amplitude and the sign of the wall shear stress at small length-scale and high frequencies, the micro-sensor is particularly suited for flow separation detection and flow control. The micro-sensor was calibrated in static and dynamic in a turbulent boundary layer wind tunnel. Several micro-sensors were embedded in various configurations for measuring the shear stress and detecting flow separation. Specially, one was embedded inside an actuator slot for in situ measurements and twelve, associated with miniaturized electronics, were implemented on a flap model for active flow control experiments.

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2

Reynard-Carette, C., G. Kohse, J. Brun, M. Carette, A. Volte, and A. Lyoussi. "Review of Nuclear Heating Measurement by Calorimetry in France and USA." EPJ Web of Conferences 170 (2018): 04019. http://dx.doi.org/10.1051/epjconf/201817004019.

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This paper gives a short review of sensors dedicated to measuring nuclear heating rate inside fission reactors in France and USA and especially inside Material Testing Reactors. These sensors correspond to heat flow calorimeters composed of a single calorimetric cell or of two calorimetric cells at least with a reference cell to obtain a differential calorimeter. The aim of this paper is to present the common running principle of these sensors and their own special characteristics through their design, calibration methods, and in-pile measurement techniques, and to describe multi-sensor probes including calorimeters.

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3

WU, M., and A. MICHELI. "Calorimetric hydrocarbon sensor for automotive exhaust applications." Sensors and Actuators B: Chemical 100, no. 3 (May 15, 2004): 291–97. http://dx.doi.org/10.1016/j.snb.2003.11.010.

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4

Muramatsu, H., J. M. Dicks, and I. Karube. "Integrated-circuit bio-calorimetric sensor for glucose." Analytica Chimica Acta 197 (1987): 347–52. http://dx.doi.org/10.1016/s0003-2670(00)84749-2.

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5

Kitsos, Vasileios, Andreas Demosthenous, and Xiao Liu. "A Smart Dual-Mode Calorimetric Flow Sensor." IEEE Sensors Journal 20, no. 3 (February 1, 2020): 1499–508. http://dx.doi.org/10.1109/jsen.2019.2946759.

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6

GAO, DONG-HUI, MING QIN, and HAI-YANG CHENG. "DESIGN AND FABRICATION OF A ONE-DIMENSIONAL SILICON FLOW SENSOR." International Journal of Information Acquisition 01, no. 04 (December 2004): 321–26. http://dx.doi.org/10.1142/s0219878904000318.

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In this paper, the influence of the geometry design on the output of a calorimetric sensor is given. The sensitivity and the range of the flow velocity are two key features for the calorimetric sensor considered here. An optimized geometry of the flow sensor is obtained and a sensor has been fabricated using the optimum geometry. Finally the experimental results are compared to the simulation results and a good agreement between them is achieved where the maximum error in flow velocity measurement is no more than 0.4 m/s.

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7

Jones, Rhys, Julian William Gardner, Andrea deLuca, Giorgia Longobardi, and Florin Udrea. "GaN-on-Si Calorimetric Thermal Conductivity Gas Sensor." ECS Meeting Abstracts MA2020-01, no. 30 (May 1, 2020): 2261. http://dx.doi.org/10.1149/ma2020-01302261mtgabs.

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8

Socorro, F., A. Mariano, and M. Rodríguez de Rivera. "Model of a calorimetric sensor for medical application." Journal of Thermal Analysis and Calorimetry 92, no. 1 (April 2008): 83–86. http://dx.doi.org/10.1007/s10973-007-8740-1.

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9

Socorro, F., and M. Rodríguez de Rivera. "Development of a calorimetric sensor for medical application." Journal of Thermal Analysis and Calorimetry 99, no. 3 (November 5, 2009): 799–802. http://dx.doi.org/10.1007/s10973-009-0568-4.

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10

Jesús, Ch, F. Socorro, and M. Rodriguez de Rivera. "Development of a calorimetric sensor for medical application." Journal of Thermal Analysis and Calorimetry 113, no. 3 (October 10, 2012): 1003–7. http://dx.doi.org/10.1007/s10973-012-2701-z.

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11

Jesús, Ch, F. Socorro, and M. Rodríguez de Rivera. "Development of a calorimetric sensor for medical application." Journal of Thermal Analysis and Calorimetry 113, no. 3 (October 17, 2012): 1009–13. http://dx.doi.org/10.1007/s10973-012-2702-y.

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12

Jesús, Ch, F. Socorro, H. J. Rodriguez de Rivera, and M. Rodriguez de Rivera. "Development of a calorimetric sensor for medical application." Journal of Thermal Analysis and Calorimetry 116, no. 1 (December 13, 2013): 151–55. http://dx.doi.org/10.1007/s10973-013-3571-8.

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13

Volte, A., C. Reynard-Carette, J. Brun, C. De Vita, M. Carette, T. Fiorido, A. Lyoussi, D. Fourmentel, J.-F. Villard, and P. Guimbal. "Study of the Flow Temperature and Ring Design Influence on the Response of a New Reduced-Size Calorimetric Cell for Nuclear Heating Quantification." EPJ Web of Conferences 170 (2018): 04026. http://dx.doi.org/10.1051/epjconf/201817004026.

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This paper concerns experimental studies of different designs of a new compact calorimetric cell under laboratory conditions. This kind of cell is used for the measurement of the nuclear heating rate inside Material Testing Reactors thanks to differential calorimetry. The results, obtained by applying an operating protocol corresponding to a preliminary out-of-pile calibration step, are presented for three designs. The influence of the horizontal-fin design is shown on the calibration curve and the sensor sensitivity. The influence of the external fluid flow temperature is given for the quarter design. The different responses of the calorimetric cell are explained by taken into account a 1D analytical thermal model coupling thermal conductive and radiative transfers.

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14

Porkovich, A. J., M. D. Arnold, G. Kouzmina, B. Hingley, A. Dowd, and M. B. Cortie. "Calorimetric Sensor for Use in Hydrogen Peroxide Aqueous Solutions." Sensor Letters 9, no. 2 (April 1, 2011): 695–97. http://dx.doi.org/10.1166/sl.2011.1594.

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15

Rodríguez de Rivera, P. J., Mi Rodríguez de Rivera, F. Socorro, M. Rodríguez de Rivera, and G. M. Callicó. "Human skin thermal properties determination using a calorimetric sensor." Journal of Thermal Analysis and Calorimetry 142, no. 1 (April 9, 2020): 461–71. http://dx.doi.org/10.1007/s10973-020-09627-6.

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16

Nebhen, Jamel, Khaled Alnowaiser, and Sofiene Mansouri. "Constant Temperature Anemometer with Self-Calibration Closed Loop Circuit." Applied Sciences 10, no. 10 (May 14, 2020): 3405. http://dx.doi.org/10.3390/app10103405.

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In this paper, a Micro-Electro-Mechanical Systems (MEMS) calorimetric sensor with its measurement electronics is designed, fabricated, and tested. The idea is to apply a configurable voltage to the sensitive resistor and measure the current flowing through the heating resistor using a current mirror controlled by an analog feedback loop. In order to cancel the offset and errors of the amplifier, the constant temperature anemometer (CTA) circuit is periodically calibrated. This technique improves the accuracy of the measurement and allows high sensitivity and high bandwidth frequency. The CTA circuit is implemented in a CMOS FD-SOI 28 nm technology. The supply voltage is 1.2 V while the core area is 0.266 mm2. Experimental results demonstrate the feasibility of the MEMS calorimetric sensor for measuring airflow rate. The developed MEMS calorimetric sensor shows a maximum normalized sensitivity of 117 mV/(m/s)/mW with respect to the input heating power and a wide dynamic flow range of 0–26 m/s. The high sensitivity and wide dynamic range achieved by our MEMS flow sensor enable its deployment as a promising sensing node for direct wall shear stress measurement applications.

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17

GELDERBLOM, H., A. VAN DER HORST, J. R. HAARTSEN, M. C. M. RUTTEN, A. A. F. VAN DE VEN, and F. N. VAN DE VOSSE. "Analytical and experimental characterization of a miniature calorimetric sensor in a pulsatile flow." Journal of Fluid Mechanics 666 (November 10, 2010): 428–44. http://dx.doi.org/10.1017/s0022112010004234.

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The behaviour of a miniature calorimetric sensor, which is under consideration for catheter-based coronary-artery-flow assessment, is investigated in both steady and pulsatile tube flows. The sensor is composed of a heating element operated at constant power and two thermopiles that measure flow-induced temperature differences over the sensor surface. An analytical sensor model is developed, which includes axial heat conduction in the fluid and a simple representation of the solid wall, assuming a quasi-steady sensor response to the pulsatile flow. To reduce the mathematical problem, described by a two-dimensional advection–diffusion equation, a spectral method is applied. A Fourier transform is then used to solve the resulting set of ordinary differential equations and an analytical expression for the fluid temperature is found. To validate the analytical model, experiments with the sensor mounted in a tube have been performed in steady and pulsatile water flows with various amplitudes and Strouhal numbers. Experimental results are generally in good agreement with theory and show a quasi-steady sensor response in the coronary-flow regime. The model can therefore be used to optimize the sensor design for coronary-flow assessment.

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18

Glatzl, Thomas, Samir Cerimovic, Harald Steiner, Almir Talic, Roman Beigelbeck, Artur Jachimowicz, Thilo Sauter, and Franz Keplinger. "Hot-film and calorimetric thermal air flow sensors realized with printed board technology." Journal of Sensors and Sensor Systems 5, no. 2 (July 19, 2016): 283–91. http://dx.doi.org/10.5194/jsss-5-283-2016.

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Abstract. This paper addresses the development of flow sensors optimized for heating, ventilating, and air conditioning systems. The sensors are based on the printed circuit board technology facilitating robust, flexible (in terms of layout), and cost-effective devices. Two approaches for measuring fluid quantities like flow velocity over the whole cross section are investigated in this context. The first one relies on hot-film transduction and stands out for its simplicity, but also shows some severe limitations, which can be circumvented by the second approach based on calorimetric transduction. Supported by extensive numerical simulations, several sensor embodiments were investigated and fabricated. After experimental characterization, measurement and simulation results were compared, which turned out to be in good agreement.

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19

Zhang, Xing, Zhijian Feng, Jianing Wang, and Shaolin Yu. "An Optimized Temperature Sensor Calorimetric Power Device Loss Measurement Method." Energies 12, no. 7 (April 8, 2019): 1333. http://dx.doi.org/10.3390/en12071333.

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In the optimized design of power converters, loss analysis of power devices is important. Compared with estimation methods, measuring the power device loss directly in the circuit under test is more accurate. The loss measurement method can be divided into two categories: electrical measurement and calorimetric measurement. The accuracy of the electrical measurement result is restricted to the accuracy of the measurement equipment and parasitic parameters, especially for fast switching devices like SiC devices. The results obtained from calorimetric measurement are more convincing. Based on the measurement principle, calorimetric measurement can be divided into four categories: flow density measurement, temperature equivalent measurement, double jacket measurement, and temperature sensor measurement. This paper proposes an optimized temperature sensor measurement method, which has shorter time consumption, a simpler setup, and lower cost. The principles of the optimized method are described and compared with the traditional ways in detail to show its advantages. The loss measurement and error analysis are carried out in a three-level ANPC (active neutral-point-clamped) topology experiment platform based on the SiC&Si hybrid module to prove the accuracy and practicability of this method.

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20

Weiss, Julien, Quentin Schwaab, Yacine Boucetta, Alain Giani, Céline Guigue, Philippe Combette, and Benoît Charlot. "Simulation and testing of a MEMS calorimetric shear-stress sensor." Sensors and Actuators A: Physical 253 (January 2017): 210–17. http://dx.doi.org/10.1016/j.sna.2016.11.018.

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21

Erck, R. A., and R. Paitich. "Measurements of ion-beam dose rate with a calorimetric sensor." Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms 47, no. 4 (June 1990): 462–65. http://dx.doi.org/10.1016/0168-583x(90)90627-7.

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22

Enoki, Toshiaki, Keishi Matsuo, Joji Ohshita, and Yousuke Ooyama. "Synthesis and optical and electrochemical properties of julolidine-structured pyrido[3,4-b]indole dye." Physical Chemistry Chemical Physics 19, no. 5 (2017): 3565–74. http://dx.doi.org/10.1039/c6cp08573c.

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23

Rodríguez de Rivera, Pedro Jesús, Miriam Rodríguez de Rivera, Fabiola Socorro, Manuel Rodríguez de Rivera, and Gustavo Marrero Callicó. "A Method to Determine Human Skin Heat Capacity Using a Non-Invasive Calorimetric Sensor." Sensors 20, no. 12 (June 17, 2020): 3431. http://dx.doi.org/10.3390/s20123431.

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A calorimetric sensor has been designed to measure the heat flow dissipated by a 2 × 2 cm2 skin surface. In this work, a non-invasive method is proposed to determine the heat capacity and thermal conductance of the area of skin where the measurement is made. The method consists of programming a linear variation of the temperature of the sensor thermostat during its application to the skin. The sensor is modelled as a two-inputs and two-outputs system. The inputs are (1) the power dissipated by the skin and transmitted by conduction to the sensor, and (2) the power dissipated in the sensor thermostat to maintain the programmed temperature. The outputs are (1) the calorimetric signal and (2) the thermostat temperature. The proposed method consists of a sensor modelling that allows the heat capacity of the element where dissipation takes place (the skin) to be identified, and the transfer functions (TF) that link the inputs and outputs are constructed from its value. These TFs allow the determination of the heat flow dissipated by the surface of the human body as a function of the temperature of the sensor thermostat. Furthermore, as this variation in heat flow is linear, we define and determine an equivalent thermal resistance of the skin in the measured area. The method is validated with a simulation and with experimental measurements on the surface of the human body.

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24

de Rivera, Pedro Jesús Rodríguez, Miriam Rodríguez de Rivera, Fabiola Socorro, and Manuel Rodríguez de Rivera. "Measurement of human body surface heat flux using a calorimetric sensor." Journal of Thermal Biology 81 (April 2019): 178–84. http://dx.doi.org/10.1016/j.jtherbio.2019.02.022.

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25

Weiss, Julien, Emmanuel Jondeau, Alain Giani, Benoît Charlot, and Philippe Combette. "Static and dynamic calibration of a MEMS calorimetric shear-stress sensor." Sensors and Actuators A: Physical 265 (October 2017): 211–16. http://dx.doi.org/10.1016/j.sna.2017.08.048.

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26

Lee, Dongkyu, Kyo Seon Hwang, Seonghwan Kim, and Thomas Thundat. "Rapid discrimination of DNA strands using an opto-calorimetric microcantilever sensor." Lab Chip 14, no. 24 (September 23, 2014): 4659–64. http://dx.doi.org/10.1039/c4lc01000k.

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27

Persson, A., V. Lekholm, G. Thornell, and L. Klintberg. "A high-temperature calorimetric flow sensor employing ion conduction in zirconia." Applied Physics Letters 106, no. 19 (May 11, 2015): 194103. http://dx.doi.org/10.1063/1.4921051.

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28

Wang, Bin, and Qiao Lin. "A MEMS Differential-Scanning-Calorimetric Sensor for Thermodynamic Characterization of Biomolecules." Journal of Microelectromechanical Systems 21, no. 5 (October 2012): 1165–71. http://dx.doi.org/10.1109/jmems.2012.2203788.

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29

Xu, Wei, Shenhui Ma, Xiaoyi Wang, Yi Chiu, and Yi-Kuen Lee. "A CMOS-MEMS Thermoresistive Micro Calorimetric Flow Sensor With Temperature Compensation." Journal of Microelectromechanical Systems 28, no. 5 (October 2019): 841–49. http://dx.doi.org/10.1109/jmems.2019.2928317.

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30

Rodriguez de Rivera, Pedro Jesús, Miriam Rodriguez de Rivera, Fabiola Socorro, and Manuel Rodriguez de Rivera. "Calibration and operation improvements of a calorimetric sensor for medical applications." Measurement 186 (December 2021): 110134. http://dx.doi.org/10.1016/j.measurement.2021.110134.

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31

Djuzhev, Nikolay A., Dmitry Novikov, and Vladimir Ryabov. "Application of the Streamlined Body for Properties Amplification of Thermoresistive MEMS Gas Flow Sensor." Solid State Phenomena 245 (October 2015): 247–52. http://dx.doi.org/10.4028/www.scientific.net/ssp.245.247.

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The main problems of the gas flow meters are the improvement of the sensitivity and velocity range. In this paper thermoresistive membrane gas flow sensor is considered. The sensor is based on the calorimetric principle of operation and developed for the thermal gas flow meters. Special streamlined body was used to improve sensor’s characteristics. It is shown that streamlined body raises sensitivity by 2 times and improves velocity range of the sensor.

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32

Freire, R. C. S., G. S. Deep, P. C. Lobo, A. M. N. Lima, J. S. Rocha Neto, and A. Oliveira. "Dynamic Response of a Feedback Thermoresistive Electrical Substitution Pyranometer." Journal of Solar Energy Engineering 120, no. 2 (May 1, 1998): 126–30. http://dx.doi.org/10.1115/1.2888055.

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Calorimetric pyranometers use plane black thermal sensors which absorb solar radiation. If a thermoresistive transducer (sensor-detector combination) is used, the temperature measured is nearer the true value than for thermoelectric transducers. More importantly, the measurement of electrical power is much more accurate than the measurement of temperature. In commercial platinum (thermoresistive), thin film thermometers, the substrate produces transducer time constants an order of magnitude larger than for the best thermoelectric transducers. Use of an electronic amplifier with the thermoresistive sensor, forming one arm of a Wheatstone bridge and arranged in a negative feedback configuration, can reduce the overall response time considerably. Theoretical formulations of instrument response, taking into account the amplifier input offset voltage, are presented and the response time is estimated.

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33

Zverev, A. V., M. Andronik, V. V. Echeistov, Z. H. Issabayeva, O. S. Sorokina, T. Konstantinova, E. S. Lotkov, I. A. Ryzhikov, and I. A. Rodionov. "Integrated Microfluidic Flow Sensor for LAB-oN-CHIP and PoINT-oF-CARE Applications." Biotekhnologiya 36, no. 4 (2020): 112–20. http://dx.doi.org/10.21519/0234-2758-2020-36-4-112-120.

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The results of the development and manufacture of an integrated membrane-free sensor for the control of accurate dilution of liquid samples on the microfluidic chip are presented. The proposed type of devices is intended for direct precise measurements of liquid flow rate in microchannels of laboratories-on-chip, including point-of-care systems. The sensor topology was optimized based on the numerical simulation results and technological requirements. The main characteristic of the developed sensor is the lack of a membrane in the design while maintaining the sensitivity and accuracy of the device at the level of a commercial membrane analogue. The fully biocompatible sensor was manufactured using standard microelectronics and soft lithography technologies. In order to optimize the sensor design, 32 different topologies of the device were tested. The integration of the flow sensors on the chip allows to significantly reduce the dead volume of the hydrodynamic system and to control the amount of liquid entering the individual reservoirs of the microfluidic chip. The sensor occupies an area of (210 x 140) um2 in the channel and is characterized by a relative error of 5% in the flow rate range of 100-1000 ul/min. microfluidics, lab-on-chip, calorimetric flow sensor, thermoresistive sensor, numerical simulation, hydrodynamics, complementary metal-oxide-semiconductor, microtechnologies Devices were made at the BMSTU Nanofabrication Facility (FMN Laboratory, FMNS REC, ID 74300).

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34

Illyaskutty, Navas, Onur Kansizoglu, Oguzhan Akdag, Binayak Ojha, Jens Knoblauch, and Heinz Kohler. "Miniaturized Single Chip Arrangement of a Wheatstone Bridge Based Calorimetric Gas Sensor." Chemosensors 6, no. 2 (May 19, 2018): 22. http://dx.doi.org/10.3390/chemosensors6020022.

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35

Greve, A., J. Olsen, N. Privorotskaya, L. Senesac, T. Thundat, W. P. King, and A. Boisen. "Micro-calorimetric sensor for vapor phase explosive detection with optimized heat profile." Microelectronic Engineering 87, no. 5-8 (May 2010): 696–98. http://dx.doi.org/10.1016/j.mee.2009.12.069.

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36

Edgar, A. "Calorimetric measurements of capacitance and inductance using an integrated circuit temperature sensor." American Journal of Physics 61, no. 10 (October 1993): 949–51. http://dx.doi.org/10.1119/1.17375.

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37

Sun, Zhongsheng, Yongxi Shen, Changrong Yuan, and Xiaoning Li. "Influence of contamination on measurement accuracy of the calorimetric air flow sensor." Measurement 145 (October 2019): 108–17. http://dx.doi.org/10.1016/j.measurement.2019.05.073.

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38

Jildeh, Zaid B., Patrick Kirchner, Jan Oberländer, Alexander Kremers, Torsten Wagner, Patrick H. Wagner, and Michael J. Schöning. "FEM-based modeling of a calorimetric gas sensor for hydrogen peroxide monitoring." physica status solidi (a) 214, no. 9 (May 22, 2017): 1600912. http://dx.doi.org/10.1002/pssa.201600912.

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39

Xu, Wei, Bo Wang, Mingzheng Duan, Moaaz Ahmed, Amine Bermak, and Yi-Kuen Lee. "A Three-Dimensional Integrated Micro Calorimetric Flow Sensor in CMOS MEMS Technology." IEEE Sensors Letters 3, no. 2 (February 2019): 1–4. http://dx.doi.org/10.1109/lsens.2019.2893151.

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40

Glatzl, Thomas, Roman Beigelbeck, Samir Cerimovic, Harald Steiner, Florian Wenig, Thilo Sauter, Albert Treytl, and Franz Keplinger. "A Thermal Flow Sensor Based on Printed Circuit Technology in Constant Temperature Mode for Various Fluids." Sensors 19, no. 5 (March 2, 2019): 1065. http://dx.doi.org/10.3390/s19051065.

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We present a thermal flow sensor designed for measuring air as well as water flow velocities in heating, ventilation, and air conditioning (HVAC) systems. The sensor is designed to integrate the flow along the entire diameter of the pipe also quantifying the volume flow rate of the streaming fluid where the calorimetric principle in constant temperature operation is utilized as a readout method. In the constant temperature mode, a controller keeps a specific excess temperature between sensing elements at a constant level resulting in a flow dependent heater voltage. To achieve cost-effective sensors, the fabrication of the transducer is fully based on printed circuit board technology allowing low-cost mass production with different form factors. In addition, 2D-FEM simulations were carried out in order to predict the sensor characteristic of envisaged setups. The simulation enables a fast and easy way to evaluate the sensor’s behaviour in different fluids. The results of the FEM simulations are compared to measurements in real environments, proving the credibility of the model.

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41

Toda, Masaya, Ning Xia, Naoki Inomata, and Takahito Ono. "Microchanneled Calorimetric Concentration Sensor for Picoliter Liquid Samples of Cytochrome c." IEEJ Transactions on Sensors and Micromachines 137, no. 1 (2017): 28–31. http://dx.doi.org/10.1541/ieejsmas.137.28.

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42

Dhahbi, Hakim, Olivier Gallot-Lavallee, Afef Kedous-Lebouc, Patrick Mas, Olivier Geoffroy, and Sebastien Buffat. "Calorimetric measurement and modelling of iron losses in a Silicon Iron current sensor." International Journal of Applied Electromagnetics and Mechanics 59, no. 2 (March 21, 2019): 473–82. http://dx.doi.org/10.3233/jae-171022.

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43

Reyes Romero, Diego F., K. Kogan, Ali S. Cubukcu, and Gerald A. Urban. "Simultaneous flow and thermal conductivity measurement of gases utilizing a calorimetric flow sensor." Sensors and Actuators A: Physical 203 (December 2013): 225–33. http://dx.doi.org/10.1016/j.sna.2013.08.025.

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44

Ghouila-Houri, Cécile, Quentin Gallas, Eric Garnier, Alain Merlen, Romain Viard, Abdelkrim Talbi, and Philippe Pernod. "High temperature gradient calorimetric wall shear stress micro-sensor for flow separation detection." Sensors and Actuators A: Physical 266 (October 2017): 232–41. http://dx.doi.org/10.1016/j.sna.2017.09.030.

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45

Park, Nam-Hee, Takafumi Akamatsu, Toshio Itoh, Noriya Izu, and Woosuck Shin. "Calorimetric Thermoelectric Gas Sensor for the Detection of Hydrogen, Methane and Mixed Gases." Sensors 14, no. 5 (May 9, 2014): 8350–62. http://dx.doi.org/10.3390/s140508350.

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46

Rodríguez de Rivera, P. J., Mi Rodríguez de Rivera, F. Socorro, M. Rodríguez de Rivera, and G. M. Callicó. "Modelling and simulation of the operation of a calorimetric sensor for medical application." Journal of Thermal Analysis and Calorimetry 142, no. 1 (March 27, 2020): 483–92. http://dx.doi.org/10.1007/s10973-020-09554-6.

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47

Sun, Zhongsheng, Yang Wang, and Changrong Yuan. "Influence of oil deposition on the measurement accuracy of a calorimetric flow sensor." Measurement 185 (November 2021): 110052. http://dx.doi.org/10.1016/j.measurement.2021.110052.

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48

Grigoriev, Boris V. "Development of a calorimetric method for measuring the content of unfrozen water in soil at a negative temperature." Tyumen State University Herald. Physical and Mathematical Modeling. Oil, Gas, Energy 6, no. 1 (2020): 87–99. http://dx.doi.org/10.21684/2411-7978-2020-6-1-87-99.

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The paper considers the task of determining the content of unfrozen water in frozen dispersed soils. It is known that the phase transformation of pore water into a solid phase at the freezing point is subject only to free water, which is not influenced by long-range electromolecular forces between the active centers of the surface of soil particles and water molecules. Distortion of the structure of pore water, called bound, leads to a decrease in its freezing temperature, and its amount is functionally dependent on the dispersion of the soil. The presence of liquid water in an array of frozen soil leads to a decrease in its strength properties, being a determining factor at near-zero temperatures. Therefore, along with other properties of frozen soil, the content of unfrozen water is an important criterion for calculating strength, thermophysical, and mass transfer processes. To quantify the content of unfrozen water, as well as determine the dependence of humidity on temperature, the calorimetric method is usually used, with its inherent disadvantages. In the work, to solve this problem, a method was developed based on the principles of calorimetry, but fundamentally different in the way of measuring the energy of phase transformations. The essence of the method is to continuously fix the energy released from the frozen sample to a predetermined temperature using a heat flux density sensor, and to continuously measure the soil’s own temperature. The standard calorimetric test procedure was adapted to process the results of a new experimental setup. The advantages of the new method for measuring the content of unfrozen water over the traditional calorimetric method are substantiated, first of all, this is a smaller number of experiments to obtain one experimental point. The applicability of the installation for studying equilibrium and nonequilibrium freezing processes of wet soil, including those with a high salt content in pore water, is shown. Comparisons of the results obtained by the calorimetric and proposed methods for the same soil showed sufficient convergence of the data, taking into account the difficulty of reproducing the experiments.

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Li, YongJin. "Calorimetric Sensor for Ethanol Using Ni2+-nitrilotriacetic Acid (NTA) Resin Immobilized Alcohol Dehydrogenase (ADH)." Current Analytical Chemistry 16, no. 6 (August 13, 2020): 795–99. http://dx.doi.org/10.2174/1573411015666190617110233.

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Background: A simple, fast and economic analytical method for the determination of ethanol is important for clinical, biological, forensic and physico-legal purposes. Methods: Ni2+-NTA resin was used as an immobilization matrix for the simple one-step purification/ immobilization of his6-tagged ADH. Different alcohols with a concentration range of 0.5-50% V/V, namely methanol, ethanol and propanol were measured using prepared ADH enzyme thermistor. The ethanol content of Tsingtao beer was tested as a real sample containing alcohol. Reproducibility and stability of prepared ADH enzyme thermistor were also investigated by repeated measurements. Results: In comparison to the controlled pore glass (a common used support for the immobilization of enzyme) used in thermal biosensor, the use of Ni2+-NTA resin not only led to simple one-step purification/ immobilization by his6-tagged ADH binding to Ni2+-NTA resin, but also made the immobilizing supports reusable. The prepared biosensor can be used to determine ethanol and methanol by the calorimetric measurement. A linear range of 1 -32% (V/V) and 2-20% (V/V) was observed for ethanol and methanol, respectively. The detection limits were 0.3% (V/V) and 1% (V/V) for ethanol and methanol, respectively. The tested ethanol concentration of Tsingtao beer was 4.5% V/V, which is comparable with the labeled alcohol by volume (ABV) 4.80%. Conclusion: Ni2+-NTA resin, as an immobilization matrix in ET sensor, provides a simple one-step purification/immobilization for His6-tagged recombinase and a reusable immobilization matrix. The prepared biosensor exhibits good repeatability and stability. Such a new biosensor shows great promise for rapid, simple, and cost-effective analysis of ethanol and methanol, both in qualitative and in quantitative tests.

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Koehler, K. E., M. A. Famiano, C. J. Fontes, T. W. Gorczyca, M. W. Rabin, D. R. Schmidt, J. N. Ullom, and M. P. Croce. "First Calorimetric Measurement of Electron Capture in $${}^{193}$$Pt with a Transition-Edge Sensor." Journal of Low Temperature Physics 193, no. 5-6 (June 1, 2018): 1151–59. http://dx.doi.org/10.1007/s10909-018-1984-2.

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