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Relevant bibliographies by topics / Resistance Thermometer

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Academic literature on the topic 'Resistance Thermometer'

Author: Grafiati

Published: 4 June 2021

Last updated: 12 February 2022

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Journal articles on the topic "Resistance Thermometer"

1

Pearce, Jonathan V., Paul Bramley, and David Cruickshank. "Development of a driftless Johnson noise thermometer for nuclear applications." EPJ Web of Conferences 225 (2020): 03001. http://dx.doi.org/10.1051/epjconf/202022503001.

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Existing temperature sensors such as thermocouples and platinum resistance thermometers suffer from calibration drift, especially in harsh environments, due to mechanical and chemical changes (and transmutation in the case of nuclear applications). A solution to the drift problem is to use temperature sensors based on fundamental thermometry (primary thermometers) where the measured property is related to absolute temperature by a fundamental physical law. A Johnson noise thermometer is such a sensor and uses the measurement of the extremely small thermal voltage noise signals generated by any resistive element to determine temperature using the Johnson-Nyquist equation. A Johnson noise thermometer never needs calibration and is insensitive to the condition of the sensor material, which makes it ideally suited to long-term temperature measurement in harsh environments. These can include reactor coolant circuits, in-pile measurements, nuclear waste management and storage, and severe accident monitoring. There have been a number of previous attempts to develop a Johnson noise thermometer for the nuclear industry, but none have achieved commercialization because of technical difficulties. We describe the results of a collaboration between the National Physical Laboratory and Metrosol Limited, which has led to a new technique for measuring Johnson noise that overcomes the previous problems that have prevented commercialization. The results from a proof-of-principle prototype that demonstrates performance commensurate with the needs of nuclear applications is presented, together with details of progress towards the commercialization of the technology. The development partners have effected a step change in the application of primary thermometry to industrial applications and seek partners for field trials and further exploitation.

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Jamieson, Jim. "A platinum resistance thermometer." Electronics Education 1991, no. 2 (1991): 7–9. http://dx.doi.org/10.1049/ee.1991.0018.

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PALM, E. C., T. P. MURPHY, S. W. TOZER, and S. T. HANNAHS. "RECENT ADVANCES IN LOW TEMPERATURE THERMOMETRY IN HIGH MAGNETIC FIELDS." International Journal of Modern Physics B 16, no. 20n22 (August 30, 2002): 3389. http://dx.doi.org/10.1142/s0217979202014504.

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The accurate determination of the temperature of an experiment at low temperatures in high magnetic fields is difficult. We present the results of measurements made using a number of new techniques developed over the last few years. In particular we discuss the results of measurements made using a unique capacitor made with Kapton and copper in a cylindrical geometry.1 This capacitance thermometer, dubbed the "Kapacitor", is different from other low temperature thermometers in that the minimum in capacitance vs. temperature can be moved to lower temperatures (to below 20 mK) by changing the construction technique. In addition, we discuss measurements on Coulomb blockade thermometers (CBT's) that offer the possibility of true primary thermomemtry at low temperatures without any magnetic field dependence. Both of these new techniques will be compared to the standard technique of resistance thermometry using RuO chip resistors. The crucial issues of accuracy and precision, usefulness for control, and noise sensitivity will be discussed for each of these technologies. In addition, recent measurements on the magnetic behavior of RuO thermometers at low temperatures and its relationship to anomalous low field peaks in the resistance that develop at temperatures below 50 mK are also presented.

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Logvinenko, S. P., O. A. Rossoshanskii, and L. A. Oprishchenko. "Low-temperature semiconductor resistance thermometer." Measurement Techniques 31, no. 11 (November 1988): 1110–12. http://dx.doi.org/10.1007/bf00864315.

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Fu, Yifeng, Guofeng Cui, and Kjell Jeppson. "Thermal Characterization of Low-Dimensional Materials by Resistance Thermometers." Materials 12, no. 11 (May 29, 2019): 1740. http://dx.doi.org/10.3390/ma12111740.

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The design, fabrication, and use of a hotspot-producing and temperature-sensing resistance thermometer for evaluating the thermal properties of low-dimensional materials are described in this paper. The materials that are characterized include one-dimensional (1D) carbon nanotubes, and two-dimensional (2D) graphene and boron nitride films. The excellent thermal performance of these materials shows great potential for cooling electronic devices and systems such as in three-dimensional (3D) integrated chip-stacks, power amplifiers, and light-emitting diodes. The thermometers are designed to be serpentine-shaped platinum resistors serving both as hotspots and temperature sensors. By using these thermometers, the thermal performance of the abovementioned emerging low-dimensional materials was evaluated with high accuracy.

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Rosemary Taylor, H., and M. Bashir Rihawi. "The dynamic thermometer: an instrument for fast measurements with Platinum Resistance Thermometers." Transactions of the Institute of Measurement and Control 15, no. 1 (January 1993): 11–18. http://dx.doi.org/10.1177/014233129301500103.

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Liu, Wei, and Jing Li. "A Calibrator Design for Thermometer Based on Precision Thermal Resistance." Advanced Materials Research 926-930 (May 2014): 1193–96. http://dx.doi.org/10.4028/www.scientific.net/amr.926-930.1193.

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This paper describes calibration principle of the thermal resistance based thermometer, and put forward digital thermometer calibration scheme of thermal resistance. Besides, according to the detailed analysis of the factors affected the accuracy of calibration, this paper supply a measure to solve this problem. This calibration design described in the article can achieve high-precise, digital calibration of the thermal resistance thermometer.

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8

Logvinenko, S. P., and G. F. Mikhina. "Resistance thermometer of rhodium-ferrum microwire." Cryogenics 26, no. 8 (August 1986): 484–85. http://dx.doi.org/10.1016/0011-2275(86)90101-3.

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9

Golub, V. V., Yu V. Zhilin, and S. A. Rylov. "A Platinum Thin-Film Resistance Thermometer." Instruments and Experimental Techniques 61, no. 3 (May 2018): 453–58. http://dx.doi.org/10.1134/s0020441218030120.

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Stephenson, Andrew P., Adam P. Micolich, Kwan H. Lee, Paul Meredith, and Ben J. Powell. "A Tunable Metal-Organic Resistance Thermometer." ChemPhysChem 12, no. 1 (December 14, 2010): 116–21. http://dx.doi.org/10.1002/cphc.201000762.

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Dissertations / Theses on the topic "Resistance Thermometer"

1

El, Hefni Baligh Hassan. "Etalonnage dynamique des capteurs de temperature en milieu liquide." Paris, ENSAM, 1987. http://www.theses.fr/1987ENAM0010.

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Petchpong, P. "Quantitative impurities effects on temperatures of tin and aluminium fixed-point cells." Thesis, Brunel University, 2009. http://bura.brunel.ac.uk/handle/2438/3984.

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The International Temperature Scale of 1990 (ITS-90) defines the present S.I.(“System International”) means of measuring temperature. The ITS-90 uses the freezing points of metals to define temperature fixed points. It also uses long-stemplatinum resistance thermometers to interpolate between the fixed points from 660 °Cdown to 84 K (if one includes the Argon triple point). Impurities are a major source of uncertainty in the fixed point temperature (of the order of 1 mK). And a better understanding of the impurity effect is required to improve top-level metrologicalthermometry. Most historical experiments with impurities have worked at a muchhigher levels of impurities – say of the order of 100ppm - and in arrangements that are not used on a day-to-day basis in a metrology laboratory. This thesis describes the deliberate doping of tin and aluminium, each with three different impurities and the effects of these on the temperature of the tin and aluminium liquid-solid phase transitions. The impurities, of the order of 1-30 ppm,were Co, Pb and Sb in the tin and Cu, Si and Ti in the aluminium. The tin and aluminium samples were in the form of ~0.3 kg ingots that would normally be used to realise an ITS-90 fixed point. Measurements were made using equipment normally available in a metrological thermometry laboratory, rather than using specially prepared samples. The samples were chemically analysed (by Glow Discharge Mass Spectrometry(GD-MS)) before and after the doping. Using the amount of dopants introduced,and/or the chemical analysis data, the measured temperature changes were compared with those interpolated from the standard text. The experimental undoped liquid-solid transition curves were also compared against theoretical curves (calculated from atheoretical model MTDATA). The results obtained did not disagree with the Hansen interpolated values (though there was considerable uncertainty in some of the measurements (e.g. a factor of 2 ormore) due to the measurement of small changes. Within these uncertainties it indicatesthat the Sum of Individual Estimates (SIE) method of correcting for, at least, metal impurities in otherwise high purity metals remain valid. However the results also showed considerable discrepancies between the initial measured and calculated temperature shifts (based on the pre-existing impurities prior to doping) suggesting that there may be impurities that are not (separately) detected by the GD-MS method. There was evidence that the thermal history of the metal phase transitions can cause considerable segregation of some impurities, particularly those likely to increase the phase transition temperature through a peritectic (“positive” impurities), and that the effects of this segregation can be clearly seen on the shape of the melting curves of thetin doped with Sb. Some of the aluminium doped with Ti freezing curves may also show evidence of a“concave up” shape at the start of the freezing curve, as previously calculated by MTDATA, though the effect is not as pronounced. All individual phase transition measurements - made over tens of hours – were repeated at least three times and found to be reproducible, hence providing a real dataset that can be used for comparison with theoretical models still under development.

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Grossman, Hy. "A New Standard for Temperature Measurement in an Aviation Environment." International Foundation for Telemetering, 2010. http://hdl.handle.net/10150/604311.

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ITC/USA 2010 Conference Proceedings / The Forty-Sixth Annual International Telemetering Conference and Technical Exhibition / October 25-28, 2010 / Town and Country Resort & Convention Center, San Diego, California
Accurate temperature measurement is an essential requirement in modern aircraft data acquisition systems. Both thermocouples and Platinum resistance temperature detectors (RTD) are used for this purpose with the latter being both more accurate and more repeatable. To ensure that only the sensor limits the accuracy of a temperature measurement, end-to-end system accuracy forward of the sensor, should be significantly greater than that of the sensor itself. This paper describes a new digital signal processing (DSP) based system for providing precision RTD based temperature measurements with laboratory accuracy in an aviation environment. Advantages of the new system include, true 3-wire RTD measurement, linear temperature output, on-board ultra-precision resistance standards and transparent dynamic calibration.

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4

Quy, Tiffany Anne. "Characterization of micro-capillary wicking evaporators." Online access for everyone, 2006. http://www.dissertations.wsu.edu/Thesis/Fall2006/T_Quy_081806.pdf.

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Bonham, Clare. "The development of accurate stagnation temperature probes for gas turbine applications." Thesis, Loughborough University, 2015. https://dspace.lboro.ac.uk/2134/19526.

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During gas turbine development testing, measurements of the gas-path stagnation temperature are used to characterise the engine running condition and establish individual engine component performance. These measurements are typically acquired using passively ventilated thermocouple probes, which are capable of achieving absolute stagnation temperature uncertainties of approximately 0.5 %. Historically, this measurement accuracy has been considered adequate to evaluate gains in turbomachinery efficiency. However, realisable turbomachinery efficiency gains have recently become sufficiently small that an improvement in measurement accuracy is now required. This has resulted in the specification of a target absolute stagnation temperature uncertainty of 0.1 %. The research presented in this thesis focusses on the development of a new stagnation temperature probe that will achieve a measurement uncertainty close to the target value. The new probe has been designed to utilise a thin-film platinum resistance thermometer (PRT) as the temperature sensitive element. For certain aspects of gas turbine engine testing, this type of sensor offers an improvement in measurement accuracy compared to a thermocouple.

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Khedekar, Mayur. "Temperature Based Estimation of the Time-Resolved Massflux of ICE Exhaust Gas Flow." Thesis, KTH, Skolan för industriell teknik och management (ITM), 2021. http://urn.kb.se/resolve?urn=urn:nbn:se:kth:diva-300050.

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The aim ofthe study was to provideinformation and experience gained with fine wire thermocouples (TCs)or resistance wire thermometers (RWTs) temperature signals to estimate the timeresolved heat transfercoefficient. Constant current method was assumed in the study and medium used in this study was air. Here the heat balance equation has been described, different Nucorrelations and further discusses potential hurdles and difficulties one may encounter while calculating heat transfer coefficient. As asolution, the use of an appropriate heatbalance equation and lowpass filter was suggested as this provides a more accurate fitting. The investigation was carried out for Reynolds number (Re) 103 to 107 and Prandlt number (Pr) 0.734. The impact of the Re and Pr on the Nusselts number (Nu) around a cylinder was represented and all the results were compared with GT-POWER engine simulation software.
Syftet med studien var att tillhandahålla information och erfarenhet från fina trådtermoelement (TC) eller motståndstrådstermometrar (RWT) temperatursignaler för att uppskatta den tidsupplösta värmeöverföringskoefficienten. Metoden med konstant flöde antogs i studien och mediet som användes i denna studie var luft. Här har värmebalansekvationen beskrivits, olika Nu-korrelationer och diskuterat ytterligare potentiella hinder och svårigheter man kan stöta på vid beräkning av värmeöverföringskoefficienten. Som en lösning föreslogs användning av en lämplig värmebalansekvation och lågpassfilter eftersom detta ger en mer exaktpassform. Undersökningen genomfördes för Reynoldsnummer (Re) 103 till 107 och Prandlt nummer (Pr) 0,734. Effekten av Re och Pr på Nusselts-numret (Nu) runt en cylinder representerades och alla resultat jämfördes med GT-POWER-motorns simuleringsprogram.

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7

Che-ShengLin and 林哲盛. "Application of Plate Thermometer to Measure Incident Radiant Heat Flux in Fire Resistance Tests." Thesis, 2012. http://ndltd.ncl.edu.tw/handle/92144437595061371169.

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碩士
國立成功大學
機械工程學系碩博士班
100
Nowadays, there are many kinds of instruments to measure radiant heat flux, but most of them are expensive and require cooling system while measuring high-temperature objects. In this research, we design a plate thermometer (PT) which can infer the incident radiant heat flux by measuring the surface temperature. Its easy-fabrication and low-cost allow us to produce a lot so that many data points can be measured simultaneously. The purpose of this study is to discuss the influence of each parameter of PT by a series of experiments. In this study, the results of PT are compared with which obtained by heat flux meter (HFM) and simulation, and then the PT is used in full-scale fire resistance tests for fire door and fire window in order to verify its usability and performance. The innovative design of plate thermometer in this study has simpler structure and it is easily fabricated, and the conduction correction factor which represents heat loss from backside is approximately 2 W/m2K. In quasi-steady state, the results of the PT are very close to that of the calibrated HFM. The differences are all within 0.5 kW/m2. Besides, the values measured by PT would not be affected by changing size, but the proportions of heat transfer mechanism would change. The ratio of convection and conduction would increase in the small size PT. Moreover, the declining rate of view factor with distance of PT is greater than HFM, so the influence by changing distance of PT is greater than HFM. In regard to the response time, the PT needs approximately 300~500 seconds to reach quasi-steady state if the environment changes suddenly. It is also found that the time constant is lower if incident radiant heat flux or forced convection increases. On the other hand, the value obtained by plate thermometer is underestimated in forced convection, because the surface of plate is cooled by convection. Moreover, the PT is used to measure incident radiant heat flux of non-insulated (Grade B) fire doors and fire windows in full-scale fire resistance tests. The differences between PT and HFM are all within 0.5 kW/m2, so it proves that the plate thermometer can be regarded as a reliable apparatus to measure incident radiant heat flux in full-scale experiments. In this study MATLAB and FDS are also used to simulate the temperature and incident radiant heat flux of plate thermometer, and then the results are compared with experiments. In laboratory experiments, the errors of temperature and incident radiant heat flux between the PT and the HFM are low, and most are within ± 30℃ and ± 0.5 kW/m2, respectively. In full-scale experiment, the maximum error occurs in the beginning of experiment when using FDS to simulate plate temperature, and then the simulated results will be close to experimental ones as time passes through. Most of the errors are within ± 30℃. The trends of incident radiant heat flux obtained by simulations and experiments are similar to each other. Most of the errors of MATLAB are within ±1 kW/m2, and the errors of FDS are slightly higher than MATLAB. Overall, it is reliable to use MATLAB and FDS to simulate in fire resistance tests.

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Shuhendler, Adam Jason. "A Novel Lipid-based Nanotechnology Platform For Biomedical Imaging And Breast Cancer Chemotherapy." Thesis, 2012. http://hdl.handle.net/1807/36253.

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A novel, lipid-based platform nanotechnology has been designed to overcome limitations of in vivo fluorescent imaging, multidrug resistance (MDR) phenotypes hindering breast cancer chemotherapy, and shortcomings of magnetic resonance imaging (MRI) thermometry. Using this platform, three nanoparticle systems have been developed: QD-SLN (quantum dot-loaded solid lipid nanoparticles), DMsPLN (doxorubicin and mitomycin C co-loaded polymer-lipid hybrid nanoparticles), and HLN (hydrogel-lipid hybrid nanoparticles). Stealth, near-infrared emitting QD-SLN were developed for deep tissue fluorescence imaging, which were capable of extending the depth of penetration beyond 2 cm, with near complete probe clearance and good tolerability in vivo. The QD-SLN was used to evaluate the biodistribution of non-targeted SLN and actively targeted RGD-conjugated SLN. Non-targeted SLN accumulated in breast tumors and evaded liver uptake. The RGD-SLN showed prolonged retention in breast tumor neovasculature at the cost of lesser tumor accumulation due to enhanced liver uptake. With this information, a long circulating, non-targeted DMsPLN with a synergistic cancer chemotherapeutic combination of doxorubicin and mitomycin C was formulated to overcome MDR, enhancing breast cancer chemotherapy. Extensive tumor cell uptake and perinuclear trafficking of DMsPLN overcame the MDR phenotype of breast tumor cells in vitro. The DMsPLN provided the most efficacious chemotherapy reported in literature against aggressive mouse mammary tumors in vivo with significant reduction in whole animal and cardiotoxicity as compared to clinically applied liposomal doxorubicin. In establishing our tumor models, the impact of Matrigel™ on the tumor microenvironment was investigated, demonstrating altered tumor vascular and lymphatic anatomy and physiology, and significantly impacting nanomedicines assessment in mouse models of cancer. In all in vivo studies, tumors were established without use of Matrigel™. To guide thermotherapy of solid tumors, a novel HLN was formulated for use in MRI thermometry, presenting the first contrast agent capable of indicating a tunable, absolute two-point temperature window. In using specific limitations of therapeutic and imaging modalities to inform rational nanoparticle design, this lipid-based platform nanotechnology has extended the application of fluorescence imaging in vivo, enhanced the utility of nanoparticulate chemotherapeutics against breast cancer independent of MDR status, and provided novel functionality for MRI thermometry.

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Books on the topic "Resistance Thermometer"

1

Mangum, B. W. Platinum resistance thermometer calibrations. Gaithersburg, MD: U.S. Dept. of Commerce, National Bureau of Standards, 1987.

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Mangum, B. W. Platinum resistance thermometer calibrations. Gaithersburg, MD: U.S. Dept. of Commerce, National Bureau of Standards, 1987.

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Mangum, B. W. NBS measurement services: Platinum resistance thermometer calibrations. Washington, D.C: National Bureau of Standards, 1987.

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Pandey, Dhirendra K. Response time correlations for platinum resistance thermometers in flowing fluids. Hampton, Va: National Aeronautics and Space Administration, Langely Research Center, 1985.

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NAMAS. Traceability of temperature measurement: Liquid-in-glass thermometers, thermocouples, platinum resistance thermometers and radiation thermometers. 4th ed. Teddington: NAMAS, 1995.

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Fandeev, E. I. Spet͡s︡ialʹnye termometry s termopreobrazovateli͡a︡mi soprotivlenii͡a︡. Moskva: Ėnergoatomizdat, 1987.

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Rusby, R. L. Frequency dependent effects in measurements with industrial platinum resistance thermometers. Luxembourg: Commission of the European Communities, 1989.

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Ltd, Labfacility. Temperature sensing with thermocouples and resistance thermometers: A practical handbook. 2nd ed. Teddington: Labfacility, 1986.

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A, Dillon-Townes Lawrence, Alderfer David W, and Langley Research Center, eds. Evaluation of industrial platinum resistance thermometers. Hampton, Va: National Aeronautics and Space Administration, Langley Research Center, 1987.

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Olsson, S. Calibration of Fire Resistance Furnances with Plate Thermometers (Calibration of Fire Resistance Furnances with Plate Thermometers). European Communities / Union (EUR-OP/OOPEC/OPOCE), 1993.

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Book chapters on the topic "Resistance Thermometer"

1

Gooch, Jan W. "Resistance Thermometer." In Encyclopedic Dictionary of Polymers, 625. New York, NY: Springer New York, 2011. http://dx.doi.org/10.1007/978-1-4419-6247-8_9963.

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Nara, Koichi, Hideyuki Kato, and Masahiro Okaji. "A Development of a Thin Wire Resistance Thermometer with Isotropic Magneto-Resistance." In Advances in Cryogenic Engineering, 1441–45. Boston, MA: Springer US, 1992. http://dx.doi.org/10.1007/978-1-4615-3368-9_79.

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Crovini, Luigi. "Resistance Thermometers." In Sensors, 69–118. Weinheim, Germany: Wiley-VCH Verlag GmbH, 2008. http://dx.doi.org/10.1002/9783527620159.ch3.

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Mitin, V. F. "Miniature Resistance Thermometers Based on Ge Films on GaAs." In Advances in Cryogenic Engineering, 749–56. Boston, MA: Springer US, 1998. http://dx.doi.org/10.1007/978-1-4757-9047-4_93.

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Phillips, R. W. "Approximating the Resistance-Temperature Relationship of Platinum Resistance Thermometers from 20 K to 273 K." In Advances in Cryogenic Engineering, 1809–15. Boston, MA: Springer US, 2000. http://dx.doi.org/10.1007/978-1-4615-4215-5_109.

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Goszczyński, Tadeusz. "Analysing the Error of Temperature Difference Measurement with Platinum Resistance Thermometers." In Advances in Intelligent Systems and Computing, 574–83. Cham: Springer International Publishing, 2018. http://dx.doi.org/10.1007/978-3-319-77179-3_54.

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Tew, W. L., and B. W. Mangum. "New Procedures and Capabilities for the Calibration of Cryogenic Resistance Thermometers at Nist." In Advances in Cryogenic Engineering, 1019–26. Boston, MA: Springer US, 1994. http://dx.doi.org/10.1007/978-1-4615-2522-6_124.

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Goszczyński, Tadeusz. "New Method for Calculation the Error of Temperature Difference Measurement with Platinum Resistance Thermometers (PRT)." In Recent Advances in Systems, Control and Information Technology, 427–34. Cham: Springer International Publishing, 2016. http://dx.doi.org/10.1007/978-3-319-48923-0_45.

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"Resistance thermometer." In Encyclopedic Dictionary of Polymers, 834. New York, NY: Springer New York, 2007. http://dx.doi.org/10.1007/978-0-387-30160-0_9781.

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"platinum resistance thermometer." In Dictionary Geotechnical Engineering/Wörterbuch GeoTechnik, 1015. Berlin, Heidelberg: Springer Berlin Heidelberg, 2014. http://dx.doi.org/10.1007/978-3-642-41714-6_162504.

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Conference papers on the topic "Resistance Thermometer"

1

Li, Wenna, and Pan Gong. "Platinum Resistance Precision Thermometer." In 2011 International Conference on Control, Automation and Systems Engineering (CASE). IEEE, 2011. http://dx.doi.org/10.1109/iccase.2011.5997740.

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Liu, Ximin. "A Platinum Resistance Bridge Thermometer." In 2016 International Forum on Energy, Environment and Sustainable Development. Paris, France: Atlantis Press, 2016. http://dx.doi.org/10.2991/ifeesd-16.2016.71.

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Sediva, Sona, and Radek Stohl. "Uncertainty Budget for Calibration of Platinum Resistance Thermometer." In 2019 20th International Carpathian Control Conference (ICCC). IEEE, 2019. http://dx.doi.org/10.1109/carpathiancc.2019.8766029.

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Baksheeva, Yu, K. Sapozhnikava, and R. Taymanov. "P2.6 - Platinum Resistance Thermometer with Metrological Self-Check." In SENSOR+TEST Conferences 2011. AMA Service GmbH, Von-Münchhausen-Str. 49, 31515 Wunstorf, Germany, 2011. http://dx.doi.org/10.5162/sensor11/sp2.6.

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Courts, S. S., and J. K. Krause. "A new capsule platinum resistance thermometer for cryogenic use." In TEMPERATURE: ITS MEASUREMENT AND CONTROL IN SCIENCE AND INDUSTRY, VOLUME 8: Proceedings of the Ninth International Temperature Symposium. AIP, 2013. http://dx.doi.org/10.1063/1.4819534.

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Kazuaki Yamazawa, Kiyoshi Anso, and Masaru Arai. "Evaluation of a horizontal furnace for precise comparison between a radiation thermometer and a platinum resistance thermometer." In SICE Annual Conference 2007. IEEE, 2007. http://dx.doi.org/10.1109/sice.2007.4421201.

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Husaini, S. Mahmood, Riyad K. Qashu, and Robert D. Blevins. "Failure of Resistance Thermometer Devices Due to Flow-Induced Vibrations." In ASME 2005 Pressure Vessels and Piping Conference. ASMEDC, 2005. http://dx.doi.org/10.1115/pvp2005-71757.

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Resistance Thermometer Devices (RTDs) are used to monitor the temperatures in sensitive locations of process piping, such as the hot and cold legs of the primary system of pressurized water reactor nuclear power plants. The RTDs are housed in thermowells that protrude in the cold and hot leg pipes. Eight of the twelve cold leg RTDs in the San Onofre Nuclear Plant have a direct safety function in the operation of the reactor. They provide the Core Protection Calculators with two temperature measurements from each of the cold legs. During the period 1997–2004, four RTD failures occurred in the cold legs of the San Onofre Nuclear Plant. Extensive investigations showed that all of the RTD failures were caused by cracking and fracturing of the platinum wires in the sensors. There was no damage to the nozzles or thermowells of the cold leg RTDs. Also, none of the RTDs in the hot leg were damaged. These failures occurred after the Cycle 9 refueling outage, when the Reactor Coolant System thermowells were replaced due to potential cracking of the Inconel 600 material. A root cause analysis was performed to identify the reasons for the failure of the RTDs in the reactor cold leg piping. The thermowells used for both the hot and cold leg RTDs are identical. The thermowells are 11.375” (289 mm) in length. Since the thickness of the cold leg pipe is 0.75” (19.1 mm) less than the thickness of the hot leg pipe, the cold leg thermowells protrude 0.75” (19.1 mm) more into the flow stream as compared to the hot leg thermowells. The protrusion lengths of the hot and cold leg thermowells in the pipe are 2.5” (63.5 mm) and 3.25” (82.6 mm), respectively. The increased protrusion length of the thermowells in the cold leg significantly lowers their natural frequency (as compared to the hot leg thermowells), which results in vortex-induced vibrations at lower flow velocities that cause failure. Also, the increased protrusion length results in increased amplitude of vortex-induced vibration of their tip that exceeds the capability of the installed RTDs. Thus, a recommendation was made to decrease the protrusion length into the cold leg pipe from 3.25” (82.6 mm) to 2.5” (63.5 mm). Since this recommendation was implemented more than eight months ago, there have been no RTD failures in the cold legs.

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Cvitas, Ljubivoj, and Zeljko Hocenski. "Automated Measurement System for Industrial Platinum Resistance Thermometer Manufacturing Industry." In 2007 IEEE International Symposium on Industrial Electronics. IEEE, 2007. http://dx.doi.org/10.1109/isie.2007.4374801.

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Hocenski, Zeljko, Ljubivoj Cvitas, and Zeljko Lasinger. "Comparison of methods for nonlinearity correction of platinum resistance thermometer." In SICE 2008 - 47th Annual Conference of the Society of Instrument and Control Engineers of Japan. IEEE, 2008. http://dx.doi.org/10.1109/sice.2008.4655207.

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Dai, Zhenting, Elise A. Corbin, and William P. King. "Multilayer microcantilever heater-thermometer with improved thermal resistance for nanotopography measurements." In 2010 IEEE 23rd International Conference on Micro Electro Mechanical Systems (MEMS). IEEE, 2010. http://dx.doi.org/10.1109/memsys.2010.5442467.

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Reports on the topic "Resistance Thermometer"

1

Mangum, B. W. Platinum resistance thermometer calibrations. Gaithersburg, MD: National Bureau of Standards, 1987. http://dx.doi.org/10.6028/nbs.sp.250-22.

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2

Strouse, G. F. Standard Platinum Resistance Thermometer Calibrations from the Ar TP to the Ag FP. National Institute of Standards and Technology, January 2008. http://dx.doi.org/10.6028/nist.sp.250-81.

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3

Carroll, R., and R. Shepard. The Method of Construction of a Dual Johnson-Noise-Power and Resistance Thermometer for1375 K (1100° C) Service in a Vacuum Environment. Office of Scientific and Technical Information (OSTI), September 1994. http://dx.doi.org/10.2172/10200226.

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4

Carroll, R. M., and R. L. Shepard. Post-accident examination of platinum resistance thermometers installed in the TMI-2 reactor. Office of Scientific and Technical Information (OSTI), September 1985. http://dx.doi.org/10.2172/5063009.

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5

Tew, W. L., G. F. Strouse, and C. W. Meyer. A revised assessment of calibration uncertainties for capsule type standard platinum and rhodium-iron resistance thermometers. Gaithersburg, MD: National Institute of Standards and Technology, 1998. http://dx.doi.org/10.6028/nist.ir.6138.

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6

Tew Jr., Weston L. Calibration of Cryogenic Resistance Thermometers between 0.65 K and 165 K on the International Temperature Scale of 1990. National Institute of Standards and Technology, June 2015. http://dx.doi.org/10.6028/nist.sp.250-91.

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Assessment of uncertainties of calibration of resistance thermometers at the National Institute of Standards and Technology. Gaithersburg, MD: National Institute of Standards and Technology, 1994. http://dx.doi.org/10.6028/nist.ir.5319.

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