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1

Lesser, Larry. "Taking the temperature of scale type." Teaching Statistics 37, no. 1 (July 7, 2014): 6. http://dx.doi.org/10.1111/test.12061.

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Park, Donghyun, and Tae Sung Oh. "Reliability Characteristics of a Package-on-Package with Temperature/Humidity Test, Temperature Cycling Test, and High Temperature Storage Test." Journal of the Microelectronics and Packaging Society 23, no. 3 (September 30, 2016): 43–49. http://dx.doi.org/10.6117/kmeps.2016.23.3.043.

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3

TOMINAGA, Toshibumi. "High temperature hardness test." Journal of the Japan Society for Precision Engineering 55, no. 8 (1989): 1337–41. http://dx.doi.org/10.2493/jjspe.55.1337.

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4

Takamatsu, Kuniyoshi, Shohei Ueta, and Kazuhiro Sawa. "ICONE19-43224 ANALYSIS OF A LOSS OF FORCED COOLING TEST USING THE HIGH TEMPERATURE ENGINEERING TEST REACTOR (HTTR)." Proceedings of the International Conference on Nuclear Engineering (ICONE) 2011.19 (2011): _ICONE1943. http://dx.doi.org/10.1299/jsmeicone.2011.19._icone1943_92.

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5

Meister, Michael, and Marco Reinhard. "A modular application specific active test environment for high-temperature wafer test up to 300 °C." Additional Conferences (Device Packaging, HiTEC, HiTEN, and CICMT) 2019, HiTen (July 1, 2019): 000122–25. http://dx.doi.org/10.4071/2380-4491.2019.hiten.000122.

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Abstract Applications in harsh environment such as high temperatures require electronic devices for signal amplification, calculations and digital interfaces. These devices often contain ASICs (application specific integrated circuits) which are suitable for high temperatures above 125 °C. For functionality verification of these high-temperature ASICs a high-temperature wafer test environment is necessary. This article describes a high-temperature wafer test setup which can be used up to 300 °C. It is based on a modular concept for a maximum of 48 test channels. The combination of three modular components (contact needle system, thermal insulation chamber and active probe card) allows adapting the setup to different ASICs and pad layouts. The active probe card operates at temperatures below 65 °C during 300 °C wafer test temperature. It is mounted on the thermal insulation chamber for signal amplification, defined loads or generation of precise input signals. This modular concept significantly shortens the development time for the high-temperature wafer test and thus saves time and reduce the costs of ASIC development.
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6

Kerr, R. A. "Shock Test Squeezes Core Temperature." Science 267, no. 5204 (March 17, 1995): 1597–98. http://dx.doi.org/10.1126/science.267.5204.1597.

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7

Shin, Soon Gi. "Deformation Behavior of TiC-Mo Composites at High Temperature by Compression Test." Korean Journal Metals and Materials 51, no. 12 (December 5, 2013): 921–28. http://dx.doi.org/10.3365/kjmm.2013.51.12.921.

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8

Le, Quang X., Vinh TN Dao, Jose L. Torero, Cristian Maluk, and Luke Bisby. "Effects of temperature and temperature gradient on concrete performance at elevated temperatures." Advances in Structural Engineering 21, no. 8 (December 8, 2017): 1223–33. http://dx.doi.org/10.1177/1369433217746347.

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To assure adequate fire performance of concrete structures, appropriate knowledge of and models for performance of concrete at elevated temperatures are crucial yet currently lacking, prompting further research. This article first highlights the limitations of inconsistent thermal boundary conditions in conventional fire testing and of using constitutive models developed based on empirical data obtained through testing concrete under minimised temperature gradients in modelling of concrete structures with significant temperature gradients. On that basis, this article outlines key features of a new test setup using radiant panels to ensure well-defined and reproducible thermal and mechanical loadings on concrete specimens. The good repeatability, consistency and uniformity of the thermal boundary conditions are demonstrated using measurements of heat flux and in-depth temperature of test specimens. The initial collected data appear to indicate that the compressive strength and failure mode of test specimens are influenced by both temperature and temperature gradient. More research is thus required to further quantify such effect and also to effectively account for it in rational performance-based fire design and analysis of concrete structures. The new test setup reported in this article, which enables reliable thermal/mechanical loadings and deformation capturing of concrete surface at elevated temperatures using digital image correlation, would be highly beneficial for such further research.
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9

TANAKA, Toshiyuki, Minoru OHKUBO, Tatsuo IYOKU, Kazuhiko KUNITOMI, Takeshi TAKEDA, Nariaki SAKABA, and Kenji SAITO. "Performance Test of the HTTR (High Temperature Engineering Test Reactor)." Journal of the Atomic Energy Society of Japan / Atomic Energy Society of Japan 41, no. 6 (1999): 686–98. http://dx.doi.org/10.3327/jaesj.41.686.

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10

Drehmer, Timothy J. "Crossover test can detect temperature differences." Postgraduate Medicine 113, no. 6 (June 2003): 16. http://dx.doi.org/10.3810/pgm.2003.06.1442.

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11

Kim, Heetae, Youngkwon Kim, Min Ki Lee, Gunn-Tae Park, and Wookang Kim. "Low Temperature Test of HWR Cryomodule." Applied Science and Convergence Technology 25, no. 3 (May 30, 2016): 47–50. http://dx.doi.org/10.5757/asct.2016.25.3.47.

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12

Mitchell, Laura A., Raymond A. R. MacDonald, and Eric E. Brodie. "Temperature and the cold pressor test." Journal of Pain 5, no. 4 (May 2004): 233–37. http://dx.doi.org/10.1016/j.jpain.2004.03.004.

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13

Çakmak, Umut D., Imre Kallaí, and Zoltán Major. "Temperature dependent bulge test for elastomers." Mechanics Research Communications 60 (September 2014): 27–32. http://dx.doi.org/10.1016/j.mechrescom.2014.05.006.

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14

Cummins, Jim R., Jim B. Causey, and David Kapsos. "High‐temperature quiet‐flow test facility." Journal of the Acoustical Society of America 108, no. 5 (November 2000): 2526. http://dx.doi.org/10.1121/1.4743347.

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15

Caruso, Hank. "Rationale for Durability Temperature Test Compression." Journal of the IEST 39, no. 1 (January 31, 1996): 33–40. http://dx.doi.org/10.17764/jiet.2.39.1.uj1040631855671w.

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This paper describes temperature test compression strategy suitable for use with either commercial or military electronic products. An example, with calculations and supporting rationale, is presented for developing an accelerated temperature test profile for a representative electronics product based on actual conditions in its service environment. Both operating and nonoperating periods are considered over a full range of hot, cold, sunny, and cloudy days. Test compression is based on equivalent amounts of fatigue accumulation in the test laboratory and in actual service. Significant assumptions and variables that can affect estimates of fatigue accumulation and test validity are also discussed.
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16

Petersen, D., DL Shelleman, OM Jadaan, DP Butt, RE Tressler, JR Hellmann, and JJ Mecholsky. "High Temperature Tube Burst Test Apparatus." Journal of Testing and Evaluation 20, no. 4 (1992): 275. http://dx.doi.org/10.1520/jte11723j.

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17

Chepel, V. Y., H. M. Araujo, M. I. Lopes, R. Ferreira Marques, and A. J. P. L. Policarpo. "Low temperature test of photomultiplier tubes." Applied Radiation and Isotopes 46, no. 6-7 (June 1995): 495–96. http://dx.doi.org/10.1016/0969-8043(95)00067-4.

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18

Réger, Mihály, Balázs Verő, Zsolt Csepeli, and Péter Pinke. "Intercritical Interrupted Jominy Test." Materials Science Forum 537-538 (February 2007): 549–54. http://dx.doi.org/10.4028/www.scientific.net/msf.537-538.549.

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The final microstructure of DP and TRIP assisted steels can evolve after hot working (hot rolling) or during post heat treatment process. In the formation of the final structure a number of different technological parameters have important role, e.g. finishing temperature of rolling, cooling rates, temperature of intercritical annealing, etc. As a result of the individual factors and their combinations a lot of production technology routes are feasible. The effect of the different combinations of these technological parameters on the microstructure can be mapped by a special Jominy end-quench test (so called intercritical Jominy end-quench test) described in this paper. Unlike the traditional Jominy test, in this case there is a partial austenizing between A1 and A3 temperatures which results in a given amount of ferrite in the microstructure before quenching. The amount of ferrite depends on the temperature. In some cases the quenching process was interrupted for a given period of time in order to model the cooling process on the run-out table. During cooling each point of the Jominy specimen has a different cooling rate, so the effect of cooling rate on the microstructure can be evaluated along the length of the specimen.
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19

Kon, Hirokazu, and Hideki Saito. "Test of the temperature difference model predicting masting behavior." Canadian Journal of Forest Research 45, no. 12 (December 2015): 1835–44. http://dx.doi.org/10.1139/cjfr-2015-0118.

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The differential temperature (ΔT) model, based on the assumption that masting plants respond to the difference in the temperatures during the growing seasons 1 and 2 years prior to seed production, has recently been proposed to explain the proximate factor of masting. In this study, we used a 28-year series of data on pollen cone and seed production in Cryptomeria japonica D. Don in Japan and compared several models based on temperatures and resources to test whether ΔT acts as a cue or is a proxy for resource limitation. Of all the models tested, models including ΔT, previous summer absolute temperature Tn–1, and reproduction in the previous year provided the best fit. The number of pollen cones and seeds produced was proportional to the difference in the mean daily maximum temperature during June to August between the preceding two years. In addition, to test whether the double mast events in consecutive years was less common than consecutive warm summers, we used our dataset and 12 datasets of pollen dispersal of 17 years or longer of C. japonica in Japan. Although consecutive warm summers occurred in 4.4% of pairs, double mast events occurred in 1.0%. The ΔT model was a considerably better predictor of the rare phenomenon of double mast events, which occur only after a specific sequence of cold–moderate–hot absolute summer temperatures. Thus, ΔT acts as cue for masting in C. japonica.
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20

Roes Lie, Indra Syahputra, Joshita Djajadisastra, and Fadlina Chany Saputri. "GREEN TEA EXTRACT IN AN EYELASH GROWTH ENHANCER GEL FORMULATION: STABILITY TEST, EYE IRRITATION TEST, AND HUMAN EYELASH GROWTH ACTIVITY." Asian Journal of Pharmaceutical and Clinical Research 10, no. 6 (June 1, 2017): 243. http://dx.doi.org/10.22159/ajpcr.2017.v10i6.18605.

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Objective: To formulate a green tea extract (GTE), which is often used as a hair growth product, to produce an eyelash gel with good stability, effectiveness, and safety for growing eyelashes.Methods: GTE was formulated into a gel. A stability test was performed at a high temperature (40±2°C), room temperature (25±2°C), low temperature (4±2°C), and a cycling temperature. An in vitro hen’s egg test-chorioallantoic membrane assay was performed to evaluate potential eye irritation. An eyelash growth test was conducted by length measurement using an eyelash ruler before and after 2 mo of application in human volunteers. Results: The GTE gel was stable in storage at high, room, and low temperatures and at cycling temperatures and did not cause eye irritation. Eyelashes grew significantly more in the test group than in the placebo group after 2 mo of application (p<0.05). Conclusion: GTE gel provides a new, safe, and effective option for growing natural eyelashes.
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21

Yi, Kyong-hwa, and Hayoung Song. "Development and Usability Test of Baby Vest Prototypes with a Body Temperature Sensing Function." Journal of the Korean Society of Clothing and Textiles 44, no. 3 (June 30, 2020): 427–40. http://dx.doi.org/10.5850/jksct.2020.44.3.427.

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22

BABA, Osamu, Kazuhiko KUNITOMI, Tatsuo IYOKU, and Haruyoshi MOGI. "Rise to Power Test Program of High Temperature Engineering Test Reactor." Proceedings of the JSME annual meeting 2000.4 (2000): 399–400. http://dx.doi.org/10.1299/jsmemecjo.2000.4.0_399.

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23

Takada, Shoji, Kazuhiko Iigaki, Masanori Shinohara, Daisuke Tochio, Yosuke Shimazaki, Masato Ono, Shunki Yanagi, et al. "Near term test plan using HTTR (high temperature engineering test reactor)." Nuclear Engineering and Design 271 (May 2014): 472–78. http://dx.doi.org/10.1016/j.nucengdes.2013.12.018.

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24

Chao, Kenneth K., Douglas K. Toth, and Costandy S. Saba. "An Integrated Test Method for High-Temperature Liquid Lubricants: Dynamic Test." Tribology Transactions 37, no. 2 (January 1994): 293–98. http://dx.doi.org/10.1080/10402009408983295.

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25

Chao, Kenneth K., and Costandy S. Saba. "An Integrated Test Method for High-Temperature Liquid Lubricants: Static Test." Tribology Transactions 38, no. 1 (January 1995): 69–74. http://dx.doi.org/10.1080/10402009508983382.

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26

Chen, Xuan, and Mansour Solaimanian. "Effect of Test Temperature and Displacement Rate on Semicircular Bend Test." Journal of Materials in Civil Engineering 31, no. 7 (July 2019): 04019104. http://dx.doi.org/10.1061/(asce)mt.1943-5533.0002753.

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27

Wang, Hong Wei, Jun Liu, Hai Qing Xiao, and Chao Wang. "Investigation of Impact Test of Power Battery under Different Environment Temperatures." Applied Mechanics and Materials 229-231 (November 2012): 1064–67. http://dx.doi.org/10.4028/www.scientific.net/amm.229-231.1064.

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The impact tests are generally performed at room temperature in actual standards, but in fact, the power battery work in variety of different environment temperatures. Therefore, the impact tests of the power battery were researched at different environment temperatures (-30°C, 20°C, 40°C and 65°C). The results showed that the impact can induce the internal short circuit, at the same time, if battery system is kept running at high environment temperature, the exothermic effect will induce the heat accumulation inside the battery, leading to thermal runaway and even the battery burning and explosion. The other result is that the higher the environment temperature is, the worse the battery thermal stability is. Temperature rise rate and maximum temperature was a linear relationship of the samples that did not burn during impact tests. And the temperature rise rate and maximum temperature was the cubic polynomial relationship of the samples that burn during impact tests. That is to say, the battery is prone to induce thermal runaway when the temperature rise rate is high.
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28

Suttner, Sebastian, and Marion Merklein. "Cyclic Tension Test of AZ31 Magnesium Alloy at Elevated Temperature Realized in a Miniaturized Uniaxial Tensile Test Setup." Materials Science Forum 854 (May 2016): 112–17. http://dx.doi.org/10.4028/www.scientific.net/msf.854.112.

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The use of new materials, e.g. aluminum and magnesium alloys, in the automotive and aviation sector is becoming increasingly important to reach the global aim of reduced emissions. Especially magnesium alloys with their low density offer great potential for lightweight design. However, magnesium alloys are almost exclusively formable at elevated temperatures. Therefore, material characterization methods need to be developed for determining the mechanical properties at elevated temperatures. In particular, cyclic tests at elevated temperatures are required to identify the isotropic-kinematic hardening behavior, which is important for numerically modeling the springback behavior. In this contribution, a characterization method for determining the cyclic behavior of the magnesium alloy AZ31B at an elevated temperature of 200 °C is presented. The setup consists of a miniaturized tensile specimen and stabilization plates to prevent buckling under compressive load. The temperature in the relevant area is introduced with the help of conductive heating. Moreover, the complex kinematic model according to Chaboche and Rousselier is identified, to map the transient hardening behavior of AZ31B after load reversal, which cannot be modeled with a single Bauschinger coefficient.
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29

Chen, Fubing, Yujie Dong, and Zuoyi Zhang. "Temperature Response of the HTR-10 during the Power Ascension Test." Science and Technology of Nuclear Installations 2015 (2015): 1–13. http://dx.doi.org/10.1155/2015/302648.

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The 10 MW High Temperature Gas-Cooled Reactor-Test Module (HTR-10) is the first High Temperature Gas-Cooled Reactor in China. With the objective of raising the reactor power from 30% to 100% rated power, the power ascension test was planned and performed in January 2003. The test results verified the practicability and validity of the HTR-10 power regulation methods. In this study, the power ascension process is preliminarily simulated using the THERMIX code. The code satisfactorily reproduces the reactor transient parameters, including the reactor power, the primary helium pressure, and the primary helium outlet temperature. Reactor internals temperatures are also calculated and compared with the test values recorded by a number of thermocouples. THERMIX correctly simulates the temperature variation tendency for different measuring points, with good to fair agreement between the calculated temperatures and the measured ones. Based on the comparison results, the THERMIX simulation capability for the HTR-10 dynamic characteristics during the power ascension process can be demonstrated. With respect to the reactor safety features, it is of utmost importance that the maximum fuel center temperature during the test process is always much lower than the fuel temperature limit of 1620°C.
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30

Beges, G. "Modeling of Temperature Conditions Between Temperature Artifact and Black Test Corner." International Journal of Thermophysics 32, no. 11-12 (November 16, 2011): 2325–32. http://dx.doi.org/10.1007/s10765-011-1123-7.

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31

Jansen, M., T. Schulenberg, and D. Waldinger. "Shop Test Result of the V64.3 Gas Turbine." Journal of Engineering for Gas Turbines and Power 114, no. 4 (October 1, 1992): 676–81. http://dx.doi.org/10.1115/1.2906641.

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The V64.3 60-MW combustion turbine is the first of a new generation of high-temperature gas turbines, designed for 50 and 60 Hz simple cycle, combined cycle, and cogeneration applications. The prototype engine was tested in 1990 in the Berlin factories under the full range of operation conditions. It was equipped with various measurement systems to monitor pressures, gas and metal temperatures, clearances, strains, vibrations, and exhaust emissions. The paper describes the engine design, the test facility and instrumentation, and the engine performance. Results are given for turbine blade temperatures, compressor and turbine vibrations, exhaust gas temperature, and NOx emissions for combustion of natural gas and fuel oil.
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32

Ramamoorthy, Praveen kumar, Florian Fischer, Han Guan, and Murad Hudda. "Material Characterization of Test Contact Pin." MATEC Web of Conferences 221 (2018): 01010. http://dx.doi.org/10.1051/matecconf/201822101010.

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Test Contact Pin is used for testing the functionality and quality of the micro-devices at extreme temperatures before shipping to customers. The contact pin transfers current & signal to the device tested through dynamic contacting where the material resistance of the pin and the contact resistance between the pin and the device plays a significant role in influencing the effectiveness of the test process. Available material specifications for these pins in the market are for ambient temperature only. The test contact pin was characterized across temperatures onto matte Sn leadframe for its contact resistance and force with respect to number of touchdowns. Contact resistance and pin force are the key variables used to understand the mechanism of the process which is also used for determining the lifespan of the contact pin. An automated and sophisticated contact tester tool (CTT) was used to characterize the test contact pin on the mattes Tin leadframe across temperatures (-43°C, 25°C and 150°C) and at fixed pin deflection. Based on the results, it was observed that the contact resistance was higher at higher temperatures. Further data analysis revealed that this phenomenon was due to influence of various factors such as temperature, leadframe material type and the material migration of Sn from leadframe to the test contact pin tip.
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33

Takahashi, A., Y. Murakami, H. Katayama, K. Ohta, and T. Okamoto. "Stabiltity test of GdTbFe at high temperature." Journal of the Magnetics Society of Japan 9, no. 2 (1985): 97–100. http://dx.doi.org/10.3379/jmsjmag.9.97.

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34

Sandén, Torbjörn, Reza Goudarzi, Michel de Combarieu, Mattias Åkesson, and Harald Hökmark. "Temperature buffer test – design, instrumentation and measurements." Physics and Chemistry of the Earth, Parts A/B/C 32, no. 1-7 (January 2007): 77–92. http://dx.doi.org/10.1016/j.pce.2006.04.025.

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35

Marsden, Timothy, Martin Stirling, and Candace Lang. "High temperature test method for polymer pipes." Polymer Testing 68 (July 2018): 309–14. http://dx.doi.org/10.1016/j.polymertesting.2018.04.008.

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36

Viiri, Jouni, and Lasse Kettunen. "Temperature profile of the Duracell■ test strip." Physics Teacher 34, no. 5 (May 1996): 276. http://dx.doi.org/10.1119/1.2344434.

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37

De Kruijf, Nico, and Rinus Rijk. "Test methods to simulate high‐temperature exposure." Food Additives and Contaminants 11, no. 2 (March 1994): 197–220. http://dx.doi.org/10.1080/02652039409374219.

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38

Delaney, Daniel E., and Michael K. Bruin. "Surface Temperature Test Methods Per IEEE 1349." IEEE Transactions on Industry Applications 43, no. 3 (2007): 821–28. http://dx.doi.org/10.1109/tia.2007.895808.

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39

Li, Yue, Ping Yang, Gerald R. North, and Andrew Dessler. "Test of the Fixed Anvil Temperature Hypothesis." Journal of the Atmospheric Sciences 69, no. 7 (July 1, 2012): 2317–28. http://dx.doi.org/10.1175/jas-d-11-0158.1.

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Abstract The fixed anvil temperature (FAT) hypothesis is examined based on the Aqua Moderate Resolution Imaging Spectroradiometer (MODIS)-based cloud-top temperature (CTT) in conjunction with the tropical atmospheric profiles and sea surface temperature (SST) from the European Centre for Medium-Range Weather Forecasts (ECMWF) Interim Reanalysis. Consistent with the physical governing mechanism of the FAT hypothesis, the peak clear-sky diabatic subsidence and convergence profiles are located at roughly the same level (200 hPa) as the peak in the cloud profile, which is fundamentally determined by the rapid decrease of water vapor concentration above this level. The geographical maxima of cloud fraction agree well with those of water vapor, clear-sky cooling rates, and diabatic convergence at 200 hPa. The use of direct CTT measurements suggests the CTT in specific Pacific basins exhibit different characteristics as the frequency distribution of the tropical SST varies from boreal winter to summer. When averaging over the tropics as a whole, the CTT distributions are approximately unchanged primarily because of cancellation by the variations associated with individual regions. An analysis of the response of the tropical mean CTT anomaly time series to the SST indicates that a possible negative relationship is present, whereas the relationship tends to be positive over the tropical western Pacific and Indian Oceans. In addition, it is suggested to interpret the FAT hypothesis, and the more recent proportionately higher anvil temperature (PHAT) hypothesis, by using the temperature at the maximum cloud detrainment level instead of the CTT.
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40

Takahashi, A., Y. Murakami, H. Katayama, K. Ohta, and T. Okamoto. "Stability Test of GdTbFe at High Temperature." IEEE Translation Journal on Magnetics in Japan 1, no. 3 (June 1985): 335–36. http://dx.doi.org/10.1109/tjmj.1985.4548584.

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41

Chatzichristodoulou, C., F. Allebrod, and M. Mogensen. "High temperature and pressure electrochemical test station." Review of Scientific Instruments 84, no. 5 (May 2013): 054101. http://dx.doi.org/10.1063/1.4807094.

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42

Eager, George, and Pater Selverstone. "4734872 Temperature control for device under test." Microelectronics Reliability 28, no. 6 (January 1988): 1001. http://dx.doi.org/10.1016/0026-2714(88)90315-0.

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43

Zhang, Ying, Bin Wang, Xinyu Liu, Ping Ni, and Wenhui Yan. "Analysis of temperature threshold in flight test." IOP Conference Series: Earth and Environmental Science 784, no. 1 (May 1, 2021): 012016. http://dx.doi.org/10.1088/1755-1315/784/1/012016.

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44

Wang, Hui Gai, Yan Pei Song, Fei Wang, and Kai Feng Zhang. "Interfacial Friction of Ceramics at High Temperature Ring-Compression Test." Materials Science Forum 704-705 (December 2011): 967–72. http://dx.doi.org/10.4028/www.scientific.net/msf.704-705.967.

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Using ring compression tests, the interfacial friction and flow stress of 3Y-TZP/Al2O3 composite at elevated temperatures were investigated. Theoretical calibration curves of the friction factor and the relative average pressure curves for the ring compression tests of 6:3:2 standard rings were drawn based on a velocity field capable of describing the bulge phenomena. The lubricant was the boron nitride (hexagonal). The tests were adopted at temperature range of 1400°C-1600°C. Results indicate that the interfacial friction factor has the value in the range of 0.34-0.49, so that boron nitride lubricant can be used effectively in present temperatures. As two extremely important parameters, the temperature and strain rate have no significant effect on the fraction factor. It is proved reliable that the ring-compression test at 1400°C and even higher is used to evaluate the performance of boron nitride lubricant.
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45

Shi, F., Li Jun Wang, Wen Fang Cui, Z. B. Li, M. Z. Xu, and Chun Ming Liu. "Hot Ductility of Fe-18Cr-12Mn-0.55N High Nitrogen Austenitic Stainless Steel." Materials Science Forum 575-578 (April 2008): 1056–61. http://dx.doi.org/10.4028/www.scientific.net/msf.575-578.1056.

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The hot ductility of Fe-18Cr-12Mn-0.55N high nitrogen austenitic stainless steel was investigated in Gleeble-2000 thermomechanical simulator. The experimental results show that the hot ductility curve of test steel is comprised of high-temperature brittlement region at the test temperatures higher than 1150°C, high-temperature ductility region at the test temperatures from 850°C to 1150°C and middle-temperature half brittlement region at the test temperatures lower than 850°C. High-temperature brittlement and middle-temperature half brittlement are caused by the appearances of δ ferrite and the precipitation of Cr2N phase at austenitic grain boundaries, respectively, and the excellent hot ductility at test temperatures between the two brittlement temperature regions results from the stable single phase austenitic microstructure.
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46

Senkerik, Vojtech, Michal Stanek, David Manas, Miroslav Manas, Adam Skrobak, and Jan Navratil. "Behavior of Recycled Material at Higher Temperature in Compression Test." Advanced Materials Research 1025-1026 (September 2014): 274–77. http://dx.doi.org/10.4028/www.scientific.net/amr.1025-1026.274.

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This research paper deals with behavior of recycled material at higher temperature. Assessment of recycled material influence takes place on four kinds of thermoplastic materials, which are always high-heat polycarbonate (PC-HT) with different amount of recycled material (pure polycarbonate, polycarbonate with twenty percent of recycled material, polycarbonate with thirty percent of recycled material and hundred percent of recycled polycarbonate). Specimens were prepared by the mostly used technology for production products, which is injection molding. Each kind of material is one by one loaded by high temperature 110°C and consequently tested. This temperature was chosen because we encounter products made with recycled material additive, which can be used at elevated temperatures. To determine behavior of recycled material at this high temperature, one basic mechanic material tests is used. This test is normalized compression test.
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47

Aly, N., M. Gomez–Heras, A. Hamed, M. Álvarez de Buergo, and F. Soliman. "The influence of temperature in a capillary imbibition salt weathering simulation test on Mokattam limestone." Materiales de Construcción 65, no. 317 (January 29, 2015): e044. http://dx.doi.org/10.3989/mc.2015.00514.

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48

Tanaka, Nobuyuki, Masahiro Nagae, Ikuo Ioka, Jin Iwatsuki, Shinji Kubo, and Kaoru Onuki. "ICONE19-43563 Corrosion test of metallic materials in high temperature acidic environments of IS process." Proceedings of the International Conference on Nuclear Engineering (ICONE) 2011.19 (2011): _ICONE1943. http://dx.doi.org/10.1299/jsmeicone.2011.19._icone1943_230.

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49

FUJIKAWA, Seigo, Minoru OHKUBO, Toshio NAKAZAWA, Kozou KAWASAKI, and Tatsuo IYOKU. "Rise-to-Power Test of the HTTR (High Temperature Engineering Test Reactor)." Transactions of the Atomic Energy Society of Japan 1, no. 4 (2002): 361–72. http://dx.doi.org/10.3327/taesj2002.1.361.

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50

Landgraf, Pierre, Peter Birnbaum, Enrique Meza-García, Thomas Grund, Verena Kräusel, and Thomas Lampke. "Jominy End Quench Test of Martensitic Stainless Steel X30Cr13." Metals 11, no. 7 (July 3, 2021): 1071. http://dx.doi.org/10.3390/met11071071.

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In this study, the influence of thermal treatments on the properties of the martensitic stainless steel X30Cr13 (EN 10088-3: 1.4028) were investigated. These steels are characterized by a high hardness as well as corrosion resistance and can be specifically adjusted by heat treatment. In particular, the austenitizing temperature ϑA and cooling rate T˙ affect the hardness and corrosion properties of martensitic stainless steels. In order to investigate these influences, the Jominy end quench tests were performed at varying austenitizing temperatures. The aim is to determine the hardness and corrosion properties as a function of the austenitizing temperature and the cooling rate. The austenitizing temperature strongly influences the solubility of alloying elements within the austenitic lattice as well as the grain size, and thus affects both precipitation and phase transformation kinetics. In consequence, different austenitizing temperatures lead to different macroscopic material properties, like hardness and pitting corrosion potential. The heat treatment was simulated using finite element (FE) method and compared with time-temperature sequences measured at different locations of the Jominy end quench sample using thermocouples. That allows determining the cooling rate T˙ between 800 ∘C and 500 ∘C and to assign it to each location of the Jominy end quench sample. The numerical estimations were in close conformity with the experimental values. By assigning the hardness and pitting corrosion potentials to the respective cooling rates as a function of the austenitizing temperature, it is possible to determine optimum process windows for the required properties.
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