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Journal articles on the topic 'Thermal Hysteresi'

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Author: Grafiati

Published: 9 March 2023

Last updated: 10 March 2023

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1

Bobenko, Nadezhda, Valeriy Egorushkin, and Alexander Ponomarev. "Hysteresis in Heat Capacity of MWCNTs Caused by Interface Behavior." Nanomaterials 12, no. 18 (September 10, 2022): 3139. http://dx.doi.org/10.3390/nano12183139.

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The paper is concerned with the study of structural disorder as well as the emergence and causes of heat capacity hysteresis in multiwall carbon nanotubes. The investigation methods are X-ray diffraction analysis, Raman spectroscopy, transmission electron microscopy, and calorimetric tests: thermogravimetric analysis, differential scanning calorimetry, and the thermal relaxation method for heat capacity hysteresis. Multiwall carbon nanotubes are shown to be composed of one or several types of zigzag–armchair domains. The domain structure of nanotube samples is responsible for the generation of uniaxial elastic microstrains and viscoelastic bending strains at domain interfaces. The thermomechanical behavior of interfaces is the chief cause of temperature hysteresis of heat capacity. The number of hystereses corresponds to the number of domain types in the structure, and values of hysteresis are determined by the crystallite size, thermal conductivity, and normal temperature distribution of strain. The found mechanism of heat capacity hysteresis can be helpful in preventing jumps in thermal properties and managing thermal memory in multiwall carbon nanotubes.

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2

Kutschan, Bernd, Silke Thoms, and Maddalena Bayer-Giraldi. "Thermal hysteresis of antifreeze proteins considering Fragilariopsis cylindrus." Algological Studies 151-152, no. 1 (September 1, 2016): 69–86. http://dx.doi.org/10.1127/algol_stud/2016/0252.

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3

Feng, Man, and Delwyn G. Fredlund. "Calibration of thermal conductivity sensors with consideration of hysteresis." Canadian Geotechnical Journal 40, no. 5 (October 1, 2003): 1048–55. http://dx.doi.org/10.1139/t03-046.

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A thermal conductivity sensor monitors soil suction by measuring the changes in thermal conductivity of the porous tip. The thermal conductivity of the porous tip is a direct function of its water content. It has long been recognized that the suction versus water content relationship of a porous material exhibits hysteresis of various magnitudes between wetting and drying processes. The sensor output may correspond to various suction values of the sensor porous tip, depending on the wetting or drying state of the porous tip. The current calibration procedure, however, represents only one of the drying processes of the sensor porous tip. A laboratory testing program was carried out to better understand the hysteretic properties of the sensor output voltage versus the suction and to further improve the calibration procedure. The output of the sensor was monitored as the sensor porous tip was subjected to various drying and wetting processes. The test results indicate an error of 30%70% for suctions higher than 100 kPa if the hysteretic effects of the porous tip are not considered in data interpretation. Based on the laboratory testing results, a revised calibration procedure was proposed that takes into consideration the capillary hysteretic effects.Key words: thermal conductivity sensor, calibration, matric suction, capillary hysteresis.

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4

Hamid, Youssef, David A. Hutt, David C. Whalley, and Russell Craddock. "Relative Contributions of Packaging Elements to the Thermal Hysteresis of a MEMS Pressure Sensor." Sensors 20, no. 6 (March 19, 2020): 1727. http://dx.doi.org/10.3390/s20061727.

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Piezoresistive silicon pressure sensor samples were thermally cycled after being consecutively packaged to three different levels. These started with the absolute minimum to allow measurement of the output and with each subsequent level incorporating additional packaging elements within the build. Fitting the data to a mathematical function was necessary both to correct for any testing uncertainties within the pressure and temperature controllers, and to enable the identification and quantification of any hysteresis. Without being subjected to any previous thermal preconditioning, the sensors were characterized over three different temperature ranges and for multiple cycles, in order to determine the relative contributions of each packaging level toward thermal hysteresis. After reaching a stabilised hysteretic behaviour, 88.5% of the thermal hysteresis was determined to be related to the bond pads and wire bonds, which is likely to be due to the large thermal mismatch between the silicon and bond pad metallisation. The fluid-fill and isolation membrane contributed just 7.2% of the total hysteresis and the remaining 4.3% was related to the adhesive used for attachment of the sensing element to the housing. This novel sequential packaging evaluation methodology is independent of sensor design and is useful in identifying those packaging elements contributing the most to hysteresis.

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5

Barrett, John. "Thermal hysteresis proteins." International Journal of Biochemistry & Cell Biology 33, no. 2 (February 2001): 105–17. http://dx.doi.org/10.1016/s1357-2725(00)00083-2.

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6

Boukheddaden, Kamel, Houcem Fourati, Yogendra Singh, and Guillaume Chastanet. "Evidence of Photo-Thermal Effects on the First-Order Thermo-Induced Spin Transition of [{Fe(NCSe)(py)2}2(m-bpypz)] Spin-Crossover Material." Magnetochemistry 5, no. 2 (April 1, 2019): 21. http://dx.doi.org/10.3390/magnetochemistry5020021.

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We have investigated by means of optical microscopy and magnetic measurements the first-order thermal spin transition of the [{Fe(NCSe)(py)2}2(m-bpypz)] spin-crossover compound under various shining intensities, far from the light-induced spin-state trapping region. We found evidence of photo-heating effects on the thermally-induced hysteretic response of this spin-crossover material, thus causing the shift of the thermal hysteresis to lower temperature regions. The experimental results are discussed in terms of the apparent crystal temperature and are analyzed theoretically using two evolution equations of motion, written on the high-spin (HS) fraction and heat balance between the crystal and the thermal bath. A very good qualitative agreement was found between experiment and theory in the stationary regime, explaining the experimental observations well and identifying the key factors governing these photo-thermal effects.

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7

Lu, Sheng, Xing Yin Zhu, Bin Liu, and Yun Peng Wang. "Effects of Workpiece Size on Temperature Distribution During FSW of AZ31 Magnesium Alloy." Materials Science Forum 850 (March 2016): 734–41. http://dx.doi.org/10.4028/www.scientific.net/msf.850.734.

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This study aims to experimentally explore the effects of varying workpiece sizes on thermal histories and temperature distributions during FSW processes of AZ31 magnesium alloy. Similar layouts of thermocouples were designed to measure thermal histories of feature points at different locations along the welding direction. A tendency of peak temperature presented that it kept climbing gradually for a distance about 60mm, then approached to change smoothly. A time hysteresis has been also found that the time of the measured temperature reaching the peak lagged behind the time of the tool staying or arriving at these feature points. The longest hysteretic time was about 6s, as the welding process proceeded, it shortened slowly. The longer the length of the welding direction was, the more obvious the tendency was, but the hysteresis, on the contrary. The intense impact of the heat accumulation was embodied in terms of the time staying above the recrystallization temperature. According to these results, it is inferred that the welding process reaches a real stable stage after the tool traversed a 60mm’s distance.

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8

Schmahl, Wolfgang W. "Athermal transformation behaviour and thermal hysteresis at the SiO2-α/ß-cristobalite phase transition." European Journal of Mineralogy 5, no. 2 (April 27, 1993): 377–80. http://dx.doi.org/10.1127/ejm/5/2/0377.

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9

GU, WEN-XIAO, MENG-LIAN ZHAO, XIAO-BO WU, MINGYANG CHEN, and QING LIU. "A HIGH-PRECISION ULTRA-LOW-POWER HYSTERETIC VOLTAGE DETECTOR USING CURRENT-BASED COMPARISON." Journal of Circuits, Systems and Computers 22, no. 09 (October 2013): 1340005. http://dx.doi.org/10.1142/s0218126613400057.

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This paper presented a high-precision, ultra-low-power hysteretic voltage detector (HVD) using current comparison to detect voltage default crossing moments for energy-harvesting systems (EHS) in wireless sensor network (WSN) applications. The HVD mainly consists of four parts: a specially designed voltage-to-current converter (VCC) with thermal stability improvement, a comparison core to make current-based comparison, a current pre-amplifier to improve its transient performance and a Schmitt inverter to provide the hysteresis characteristic. The prototype of this HVD has been implemented in SMIC 0.18 μm CMOS process and occupies 0.036 mm2 area without pads. The hysteresis window is about 120 mV wide. The temperature coefficient (TC) is about -170.2 ppm°C. The average variation to different process corners can be reduced to 1.4% by MOSFET and resistor trimming. The total power consumption is only 701.5 nW when VDD is around 1.8 V.

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10

Urrutia, Maria E., John G. Duman, and Charles A. Knight. "Plant thermal hysteresis proteins." Biochimica et Biophysica Acta (BBA) - Protein Structure and Molecular Enzymology 1121, no. 1-2 (May 1992): 199–206. http://dx.doi.org/10.1016/0167-4838(92)90355-h.

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11

Li, Zhi, Min You, Xiao Ling Zheng, Mei Rong Zhao, and Jia Ling Yan. "A FEM Study on Thermal Stress in Laminated Composite." Key Engineering Materials 373-374 (March 2008): 786–89. http://dx.doi.org/10.4028/www.scientific.net/kem.373-374.786.

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The 3-D elasto-plastic finite element method (FEM) was used to analyze the thermal stress in the laminated composite (SiC/6061Al) under the condition of a temperature cycling of 200 0C-30 0C- 200 0C-30 0C. The results from the FEM analysis showed that the hysteretic peak value of the von Mises equivalent stress in the substrate 6061Al was increased significantly as the temperature loading cycles processed on but it was nearly the same after the first cycle in the interface layer SiC of the laminated composite. The elastic strain in the substrate 6061Al varied within the range of -0.15% to 0.15% and the maximum plastic deformation was equal to about 0.26 %. The results also showed that the maximum normal stress Sx was increased from 32.8 MPa to 87.9 MPa after ten cycles and the work-hardening of the substrate 6061Al occurred during the stress and strain hysteresis loop.

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12

Kantar, Ersin. "Dynamic calculations of the core/shell structured Ising-type endohedral fullerenes: The effect of core and core/shell interaction." Modern Physics Letters B 31, no. 33 (November 27, 2017): 1750307. http://dx.doi.org/10.1142/s0217984917503079.

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In this study, we examine by comparing the dynamic magnetic and hysteretic properties of Ising-type endohedral fullerene (EF) with various dopant magnetic particles confined within a spherical cage. The model of EF X@C[Formula: see text] with X = spin-1/2, spin-1 and spin-3/2 is proposed to study the effect of the nature of core particle on the magnetic properties. The results were obtained by mean-field theory as well as Glauber-type stochastic dynamics, and focused on the response of thermal and hysteretic behaviors of systems. The system exhibits second- and first-order phase transitions. In three different core cases, the system also exhibits type-II superconductivity behavior with a dynamic hysteresis curves of the core. All results display magnetic properties of the EF which strongly depend on the nature of core particle. Moreover, core particle and core/shell (C–S) interaction are proposed as the basic factors affecting the magnetic properties of EF system.

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13

Caravelli, Francesco, Gia-Wei Chern, and Cristiano Nisoli. "Artificial spin ice phase-change memory resistors." New Journal of Physics 24, no. 2 (February 1, 2022): 023020. http://dx.doi.org/10.1088/1367-2630/ac4c0a.

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Abstract We present a proposal for realization of an electrical memory reminiscent of a memristor in connected Kagome artificial spin ice. We show that current flowing through the system alters the magnetic ensemble, which in turns controls the overall resistance thus leaving memory of current passage in the system. This introduces a current-dependent effect for a dynamic resistive state. We simulate a spin-induced thermal phase-change mechanism, and an athermal domain-wall spin inversion. In both cases we observe electrical memory behavior with an I–V hysteretic pinched loop, typical of memristors. These results can be extended to the more complex geometries in which artificial spin ice can be designed to engineer the hysteresis curve.

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14

Simonson, C. J., Y. X. Tao, and R. W. Besant. "Thermal hysteresis in fibrous insulation." International Journal of Heat and Mass Transfer 36, no. 18 (December 1993): 4433–41. http://dx.doi.org/10.1016/0017-9310(93)90127-r.

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15

Shablovskii, O. N. "Thermal hysteresis in nonlinear media." Journal of Engineering Physics 59, no. 1 (July 1990): 944–50. http://dx.doi.org/10.1007/bf00871338.

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16

Wang, Jin Song. "Irreversible Thermodynamic Discussions about Ferroelectric Phase Transitions." Advanced Materials Research 756-759 (September 2013): 4419–22. http://dx.doi.org/10.4028/www.scientific.net/amr.756-759.4419.

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The irreversibility of ferroelectric phase transitions has been studied by using the irreversible thermodynamics. The thermal hysteresis of first-order ferroelectric phase transitions and the polydomain structure of ferroelectrics can be explained on the basis of the principle of minimum entropy production. A conclusion has been derived that the thermal hysteresis is not an intrinsic property of a system in which a first-order ferroelectric phase transition occurs. The finiteness of the systems surface is connected with the thermal hysteresis.

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17

Ladjimi, A., M. Mékideche, and A. Babouri. "Thermal effects on magnetic hysteresis modeling." Archives of Electrical Engineering 61, no. 1 (January 1, 2012): 77–84. http://dx.doi.org/10.2478/v10171-012-0007-1.

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Thermal effects on magnetic hysteresis modelingA temperature dependent model is necessary for the generation of hysteresis loops of ferromagnetic materials. In this study, a physical model based on the Jiles-Atherton model has been developed to study the effect of temperature on the magnetic hysteresis loop. The thermal effects were included through a model of behavior depending on the temperature parametersMsandkof the Jiles-Atherton model. The temperature-dependent Jiles-Atherton model was validated through measurements made on ferrite material (3F3). The results have been found to be in good agreement with the model.

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18

Gutfleisch, O., T. Gottschall, M. Fries, D. Benke, I. Radulov, K. P. Skokov, H. Wende, et al. "Mastering hysteresis in magnetocaloric materials." Philosophical Transactions of the Royal Society A: Mathematical, Physical and Engineering Sciences 374, no. 2074 (August 13, 2016): 20150308. http://dx.doi.org/10.1098/rsta.2015.0308.

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Hysteresis is more than just an interesting oddity that occurs in materials with a first-order transition. It is a real obstacle on the path from existing laboratory-scale prototypes of magnetic refrigerators towards commercialization of this potentially disruptive cooling technology. Indeed, the reversibility of the magnetocaloric effect, being essential for magnetic heat pumps, strongly depends on the width of the thermal hysteresis and, therefore, it is necessary to understand the mechanisms causing hysteresis and to find solutions to minimize losses associated with thermal hysteresis in order to maximize the efficiency of magnetic cooling devices. In this work, we discuss the fundamental aspects that can contribute to thermal hysteresis and the strategies that we are developing to at least partially overcome the hysteresis problem in some selected classes of magnetocaloric materials with large application potential. In doing so, we refer to the most relevant classes of magnetic refrigerants La–Fe–Si-, Heusler- and Fe 2 P-type compounds. This article is part of the themed issue ‘Taking the temperature of phase transitions in cool materials’.

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19

Thurlow, M. S., B. J. Brooks, P. G. J. Lucas, M. R. Ardron, J. K. Bhattacharjee, and A. L. Woodcraft. "Convective instability in rotating liquid 3He-4He mixtures." Journal of Fluid Mechanics 313 (April 25, 1996): 381–407. http://dx.doi.org/10.1017/s002211209600225x.

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Thermal convection is investigated experimentally in a dilute liquid mixture of 3He in 4He at four temperatures between 20 and 100 mK above the superfluid transition temperature, chosen for their proximity to the codimension-two and hydrodynamic tricritical points. Two experimental cells of aspect ratio 2.76 and 1.00 were used. For the cell with the higher aspect ratio, two convective transitions at each of the four temperatures were observed above a critical angular velocity, and only one observed below. At temperatures lower than that of the hydrodynamic tricritical point the transition with the lower critical Rayleigh number is hysteretic for all angular velocities; above this temperature hysteresis is absent. The critical Rayleigh numbers are compared with theoretical predictions that take into account the existence of convection modes with azimuthal angular dependence. In the case of the cell with the smaller aspect ratio thermal relaxation oscillations were observed when heating from below. Convective thresholds were again observed but their critical Rayleigh numbers are almost independent of angular velocity. Some suggestions are advanced for this unexpected behaviour.

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20

Xing, Guanying, Weixian Zhao, Run Hu, and Xiaobing Luo. "Spatiotemporal Modulation of Thermal Emission from Thermal-Hysteresis Vanadium Dioxide for Multiplexing Thermotronics Functionalities." Chinese Physics Letters 38, no. 12 (December 1, 2021): 124401. http://dx.doi.org/10.1088/0256-307x/38/12/124401.

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Taking heat positively as the information carrier, thermotronics can exempt the long-lasting thermal issue of electronics fundamentally, yet has been faced with the challenging multiplexing integration of diverse functionalities. Here, we demonstrate a spatiotemporal modulation platform to achieve multiplexing thermotronics functionalities based on the thermal-hysteresis vanadium dioxide, including negative-differential thermal emission, thermal diode, thermal memristor, thermal transistor, and beyond. The physics behind the multiplexing thermotronics lies in the thermal hysteresis emission characteristics of the phase-changing vanadium dioxide during the spatiotemporal modulation. The present spatiotemporal modulation is expected to stimulate more exploration on novel functionalities, system integration, and practical applications of thermotronics.

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21

Biswas, Sourav, Pankaj Wahi, and Anjan Kumar Gupta. "Stability of thermally bistable states and their switching in superconducting weak link." Journal of Applied Physics 132, no. 14 (October 14, 2022): 144302. http://dx.doi.org/10.1063/5.0115757.

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Superconducting weak link (WL), acting as a Josephson junction (JJ), is one of the widely used elements in superconductor science and quantum circuits. A hysteretic JJ with robust switching between its superconducting and resistive state is an excellent candidate for single-photon detection. However, the ubiquitous fluctuations in the junction strongly influence the stability of the states and, thus, the transition from one to the other. Here, we present an experimental study of switching statistics of critical and retrapping currents of a JJ based on niobium WL in its hysteretic regime. The mean lifetimes of the two metastable states, namely, the zero-voltage superconducting state and finite-voltage resistive state, are estimated from the distributions. Further, close to the hysteresis crossover temperature, observed telegraphic noise in the time domain due to random switching between the states provides their lifetimes directly. We present a thermal model introducing a double-well (bistable) feature with an intriguing quantity with respect to the devices’ temperature states. The effects of temperature fluctuations on the stability of the states are shown. We discuss our results toward further improvement of the efficiency of superconducting WL or nanowire single-photon detectors.

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22

Arisawa, Mieko, Rina Iwamoto, and Masahiko Yamaguchi. "Unstable and Stable Thermal Hysteresis Under Thermal Triangle Waves." ChemistrySelect 6, no. 18 (May 10, 2021): 4461–65. http://dx.doi.org/10.1002/slct.202100089.

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23

Li, N., C. A. Andorfer, and J. G. Duman. "Enhancement of insect antifreeze protein activity by solutes of low molecular mass." Journal of Experimental Biology 201, no. 15 (August 1, 1998): 2243–51. http://dx.doi.org/10.1242/jeb.201.15.2243.

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Antifreeze proteins (AFPs) lower the non-equilibrium freezing point of water (in the presence of ice) below the melting point, thereby producing a difference between the freezing and melting points that has been termed thermal hysteresis. In general, the magnitude of the thermal hysteresis depends upon the specific activity and concentration of the AFP. This study describes several low-molecular-mass solutes that enhance the thermal hysteresis activity of an AFP from overwintering larvae of the beetle Dendroides canadensis. The most active of these is citrate, which increases the thermal hysteresis nearly sixfold from 1.2 degrees C in its absence to 6.8 degrees C. Solutes which increase activity approximately fourfold are succinate, malate, aspartate, glutamate and ammonium sulfate. Glycerol, sorbitol, alanine and ammonium bicarbonate increased thermal hysteresis approximately threefold. Interestingly, 0.5 mol l-1 sodium sulfate eliminated activity. Solute concentrations between 0.25 and 1 mol l-1 were generally required to elicit optimal thermal hysteresis activity. Glycerol is the only one of these enhancing solutes that is known to be present at these concentrations in overwintering D. canadensis, and therefore the physiological significance of most of these enhancers is unknown. The mechanism(s) of this enhancement is also unknown. The AFP used in this study (DAFP-4) is nearly identical to previously described D. canadensis AFPs. The mature protein consists of 71 amino acid residues arranged in six 12- or 13-mer repeats with a consensus sequence consisting of Cys-Thr-X3-Ser-X5-X6-Cys-X8-X9-Ala-X11-Thr-X1 3, where X3 and X11 tend to be charged residues, X5 tends to be Thr or Ser, X6 to be Asn or Asp, X9 to be Asn or Lys and X13 to be Ala in the 13-mers. DAFP-4 is shorter by one repeat than previously described D. canadensis AFPs.

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24

Wang, Zhaoyang, and Jie Wu. "A Method to Increase the Frequency Stability of a TCXO by Compensating Thermal Hysteresis." Sensors 20, no. 23 (November 28, 2020): 6812. http://dx.doi.org/10.3390/s20236812.

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Due to the rapid growth of electronic information technology, the need for the higher stability of crystal oscillators has increased. The temperature-compensated X’tal (crystal) oscillator (TCXO), a type of crystal oscillator with high frequency stability, has been widely used in communications, sensor networks, automotive electronics, industrial control, measuring devices, and other equipment. The traditional TCXO only performs frequency compensation based on the current temperature, without considering the error caused by thermal hysteresis. As the frequency stability of the TCXO improves, the thermal hysteresis of the crystal oscillator has a negligible influence on the frequency stability of the crystal oscillator. This study measured different compensation tables for hysteresis curves at different temperatures and used a microprocessor to store the historical information of crystal temperature changes. Furthermore, corresponding algorithms were designed to select the correct values, according to the temperature change history, to compensate for the thermal hysteresis of the crystal oscillator error. Experiments show that this method can reduce the hysteresis error of the crystal oscillator from 700 to 150 ppb (−40 to 80 °C).

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25

Nishikawa, K., S. Takakura, M. Nakatake, M. Yoshimura, and Y. Watanabe. "Effect of surface modification by Ar⁺ ion irradiation on thermal hysteresis of VO₂." Journal of Applied Physics 133, no. 4 (January 28, 2023): 045305. http://dx.doi.org/10.1063/5.0132957.

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Vanadium dioxide (VO2) undergoes a metal–insulator phase transition at ∼70 °C. As this is a first-order phase transition, VO2 exhibits thermal hysteresis. The reflectivity and electrical resistivity of VO2 drastically change at insulator-to-metal ( TIMT) and metal-to-insulator ( TMIT) transition temperatures during heating and cooling, respectively. For smart glass and thermal memory applications employing VO2, the origin and control factor of thermal hysteresis must be investigated. Additional elemental doping and nano-structuring of VO2 affect the thermal hysteresis width. However, the factors determining TIMT and TMIT remain unclear. TIMT and TMIT can be modified by irradiating Ar+ on the surface of VO2 nanostructures with varying Ar+ irradiation doses ( nAr+) at 1 keV. The temperature-dependent reflectivity against IR light is evaluated. For VO2, TIMT decreases with nAr+ = 3.9 × 1014 cm−2; TMIT increases with nAr+ > 3.9 × 1015 cm−2. Ar+ irradiation decreases the thermal hysteresis width. Because the expected penetration depth of Ar+ at 1 keV into the VO2 surface is <6 nm, the VO2 chemical state at the outermost surface is investigated using x-ray absorption spectroscopy with soft x-ray irradiation. The V L-edge peak energy decreases with increasing nAr+ . Ar+ irradiation reduces V only at the outermost surface state. TIMT is more sensitive than TMIT to the reduction of V. The reduction of only a small fraction at the surface affects the phase transition of the entire VO2. These results are beneficial for understanding the cause of thermal hysteresis width and improving the performance of devices using VO2.

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26

Iwasaki, Hideo. "Thermal hysteresis behaviors of thermoelectric properties." Japanese Journal of Applied Physics 53, no. 12 (November 21, 2014): 125502. http://dx.doi.org/10.7567/jjap.53.125502.

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27

Dantas, A. L., R. E. Camley, and A. S. Carrico. "Thermal Hysteresis of Thin Dy Films." IEEE Transactions on Magnetics 42, no. 10 (October 2006): 2942–44. http://dx.doi.org/10.1109/tmag.2006.878398.

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28

Zainullina, R. I., N. G. Bebenin, V. V. Mashkautsan, V. V. Ustinov, and Ya M. Mukovskii. "Giant thermal hysteresis in lanthanum manganites." Journal of Magnetism and Magnetic Materials 300, no. 1 (May 2006): e137-e139. http://dx.doi.org/10.1016/j.jmmm.2005.10.167.

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29

Demirtas, S., R. E. Camley, and A. R. Koymen. "Tunable thermal hysteresis in CoGd alloys." Applied Physics Letters 87, no. 20 (November 14, 2005): 202111. http://dx.doi.org/10.1063/1.2132530.

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30

Valerio, P. F., M. H. Kao, and G. L. Fletcher. "Thermal hysteresis activity in the skin of the cunner, Tautogolabrus adspersus." Canadian Journal of Zoology 68, no. 5 (May 1, 1990): 1065–67. http://dx.doi.org/10.1139/z90-156.

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Previous studies have shown that cunners, Tautogolabrus adspersus, remain inshore in marine waters around Newfoundland during the winter months, but are in a state of metabolic torpor, apparently surviving by undercooling without freezing. The present study reports the discovery of measurable levels of thermal hysteresis activity in aqueous extracts of winter cunner skin, but not in the blood plasma. The occurrence of a compound with thermal hysteresis activity indicates the presence of antifreeze polypeptides in the Labridae. This is of significant interest, since this family is mostly tropical in distribution, and has likely invaded northern waters in relatively recent times. The functional significance of skin thermal hysteresis activity is discussed in relation to the protective role of antifreeze compounds.

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31

Longbiao, Li. "A thermomechanical fatigue hysteresis-based damage evolution model for fiber-reinforced ceramic–matrix composites." International Journal of Damage Mechanics 28, no. 3 (April 19, 2018): 380–403. http://dx.doi.org/10.1177/1056789518772162.

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In this paper, a thermomechanical fatigue hysteresis-based damage evolution model for fiber-reinforced ceramic–matrix composites has been developed. Upon unloading and reloading, the fiber/matrix interface debonded length, interface counter-slip length, and interface new-slip length change with increasing or decreasing applied stress, which affects the stress–strain fatigue hysteresis loops and fatigue hysteresis-based damage parameters. The reloading/unloading stress–strain relationships when fiber/matrix interface partially or completely debonding are determined as a function of interface debonding/sliding, peak stress, applied cycle number, and thermal cycle temperature. The relationships between thermomechanical fatigue loading parameters (i.e. peak stress, applied cycle number, and thermal cyclic temperature), fiber/matrix interface debonding/sliding lengths, and fatigue hysteresis-based damage parameters (i.e. fatigue hysteresis dissipated energy, fatigue hysteresis modulus, and fatigue peak strain) have been established. The effects of fiber volume fraction, peak stress, matrix cracking space, and thermal cyclic temperature range on damage evolution under the out-of-phase thermomechanical cyclic loading have been discussed. The differences in damage evolution between in-phase/out-of-phase thermomechanical fatigue and isothermal fatigue loading at the same peak stress have been analyzed. The damage evolution of cross-ply SiC/magnesium aluminosilicate composite under the out-of-phase thermomechanical and isothermal fatigue loading has been predicted.

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32

Stary, O. "FORMATION OF MAGNETIC PROPERTIES OF FERRITES DURING RADIATION-THERMAL SINTERING." Eurasian Physical Technical Journal 17, no. 2 (December 24, 2020): 6–10. http://dx.doi.org/10.31489/2020no2/6-10.

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The results of a comparative analysis of the laws governing the formation of ferrite hysteresis loop parameters sintered in thermal and radiation-thermal conditions were shown. The influence of radiation exposure on the interconversion of microstructure defects and their content in ferrites, depending on the duration and temperature of treatment, was established. Also, it was shown that recrystallization grain growth under irradiation conditions is ahead of grain growth during thermal heating. The observed radiation effects were associated with the effect of radiation on the microstructure. The magnetic parameters are uniquely determined by the compaction of the sample.

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33

Bushuev, Mark B., Denis P. Pishchur, Elena B. Nikolaenkova, and Viktor P. Krivopalov. "Compensation effects and relation between the activation energy of spin transition and the hysteresis loop width for an iron(ii) complex." Physical Chemistry Chemical Physics 18, no. 25 (2016): 16690–99. http://dx.doi.org/10.1039/c6cp01892k.

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Wide thermal hysteresis loops for iron(ii) spin crossover complexes are associated with high activation barriers: the higher the activation barrier, the wider the hysteresis loop for a series of related spin crossover systems.

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34

Li, Li Fen, and Xi Xia Liang. "The Thermal Hysteresis of the Type I Antifreeze Protein ‘HPLC-6’: The Effect of Small System." Advanced Materials Research 658 (January 2013): 169–73. http://dx.doi.org/10.4028/www.scientific.net/amr.658.169.

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According to Hill’s thermodynamics theory for small system, the effect of small system on the thermal hysteresis activity of type I antifreeze protein ‘HPLC-6’ is discussed in this article. We conclude that when the solution is very dilute, the effect is not visible, and as the concentration increases, the effect becomes more visible than before, and the result also shows that the thermal hysteresis temperature becomes larger when the effect of small system is considered.

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35

Dorogina, G. A., R. I. Gulyaeva, E. N. Selivanov, V. F. Balakirev, and A. D. Vershinin. "Thermal magnetic hysteresis of nickel-doped pyrrhotites." Bulletin of the Russian Academy of Sciences: Physics 77, no. 3 (March 2013): 260–64. http://dx.doi.org/10.3103/s106287381303009x.

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Yamaguchi, Masahiko. "Thermal Hysteresis Involving Reversible Self-Catalytic Reactions." Accounts of Chemical Research 54, no. 11 (May 13, 2021): 2603–13. http://dx.doi.org/10.1021/acs.accounts.1c00090.

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37

Bushuev, Mark B. "Kinetics of spin crossover with thermal hysteresis." Physical Chemistry Chemical Physics 20, no. 8 (2018): 5586–90. http://dx.doi.org/10.1039/c7cp08554k.

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38

Vadasz, P. "Chaotic dynamics and hysteresis in thermal convection." Proceedings of the Institution of Mechanical Engineers, Part C: Journal of Mechanical Engineering Science 220, no. 3 (March 1, 2006): 309–23. http://dx.doi.org/10.1243/095440605x32101.

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The weak turbulence regime associated with non-steady and non-periodic free convection, in models allowing temporal irregular (i.e. chaotic) solutions is reviewed, and the conditions for its validity are specified. The rich dynamics linked to the transition from steady convection to chaos is demonstrated and explained analytically as well as computationally.

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39

Hoang, V. V. "Thermal hysteresis of a simulated Al2O3 system." European Physical Journal B 48, no. 4 (December 2005): 495–500. http://dx.doi.org/10.1140/epjb/e2006-00003-7.

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40

Chiou, J. A., and S. Chen. "Thermal hysteresis analysis of MEMS pressure sensors." Journal of Microelectromechanical Systems 14, no. 4 (August 2005): 782–87. http://dx.doi.org/10.1109/jmems.2005.845460.

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41

Allakhverdiev, K. R., F. A. Mikailov, A. M. Kulibekov, and N. Türetken. "Thermal hysteresis and memory effects in TIInS2." Phase Transitions 67, no. 2 (November 1998): 457–65. http://dx.doi.org/10.1080/01411599808228753.

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42

Halcrow, Malcolm A. "Spin-crossover Compounds with Wide Thermal Hysteresis." Chemistry Letters 43, no. 8 (August 5, 2014): 1178–88. http://dx.doi.org/10.1246/cl.140464.

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43

Zagainova, L., G. Klimusheva, L. Yatsenko, and V. Danilov. "Resonant-Thermal Optical Hysteresis in Liquid Crystals." Molecular Crystals and Liquid Crystals Incorporating Nonlinear Optics 192, no. 1 (January 1, 1990): 279–83. http://dx.doi.org/10.1080/00268949008035641.

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44

Rekhson, Simon M. "Thermal Stresses, Relaxation, and Hysteresis in Glass." Journal of the American Ceramic Society 76, no. 5 (May 1993): 1113–23. http://dx.doi.org/10.1111/j.1151-2916.1993.tb03728.x.

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45

Dantas, Ana L., A. S. W. T. Silva, G. O. G. Rebouças, A. S. Carriço, and R. E. Camley. "Thermal hysteresis of interface biased ferromagnetic dots." Journal of Applied Physics 102, no. 12 (December 15, 2007): 123907. http://dx.doi.org/10.1063/1.2827478.

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46

Maeda, A., T. Satake, T. Fujimori, and H. Kuroda. "Thermal hysteresis phenomena in Eu/Yb superlattices." Journal of Physics: Condensed Matter 3, no. 12 (March 25, 1991): 1967–70. http://dx.doi.org/10.1088/0953-8984/3/12/029.

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47

Gherghescu, Ioana Arina, Sorin Ciuca, Gabriela Liliana Jicmon, Ruxandra Elena Dumitrescu, and Mihai Branzei. "Thermal Cycling Influence on the Transformation Characteristics of a Ni50Ti48Nb2 Shape Memory Alloy." Revista de Chimie 68, no. 5 (June 15, 2017): 991–96. http://dx.doi.org/10.37358/rc.17.5.5596.

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The alloy was chosen in order to obtain a shape memory alloy having a wider hysteresis than equiatomic NiTi, that involves a better thermo-mechanical stability. Two samples investigated by differential scanning calorimetry (DSC) were previously annealed at 800oC/12 h and, respectively, 900 �C/12 h followed by furnace cooling. These were afterwards submitted to thermal cycling. The thermal cycling of a Ni50Ti48Nb2 alloy sample previously annealed at 900 �C/12 h results in lower critical points and higher hysteresis values as compared to those of the sample annealed at 800�C/12h, also submitted to thermal cycling. Thus, annealing a metallic part made of such an alloy at 900� C/12 h followed by thermal cycling prior to putting it into service enhances its reliability.

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48

Li, Li Fen, Lin Zhang, and Xi Xia Liang. "The Thermal Hysteresis Temperature of ‘HPLC-6’: Langmuir Model." Applied Mechanics and Materials 268-270 (December 2012): 254–57. http://dx.doi.org/10.4028/www.scientific.net/amm.268-270.254.

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The AFPs and water molecules are considered together when they adsorb on the ice surface in this article. Based on Myers and Prausnitz’s ideal adsorbed solution theory(IAST) and Langmuir adsorption model, the coverage rate of HPLC-6 on the ice surface is calculated when considering the adsorption of water, and the thermal hysteresis temperature of HPLC-6 is also given. The results show that the thermal hysteresis temperature increases as the concentration increases, and the theoretical result is agreement with experimental data.

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Łyskawiński, Wiesław, Piotr Sujka, Wojciech Szeląg, and Mariusz Barański. "Numerical analysis of hysteresis loss in pulse transformer." Archives of Electrical Engineering 60, no. 2 (June 1, 2011): 187–95. http://dx.doi.org/10.2478/v10171-011-0018-3.

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Numerical analysis of hysteresis loss in pulse transformerIn the paper, the mathematical model of coupled electromagnetic and thermal phenomena in the pulse transformer taking into account the magnetic hysteresis is presented. For the mapping of magnetic hysteresis, Jiles-Atherton model is applied. In order to solve field equations, the finite element method (FEM), "step-by-step" procedure and Newton-Raphson algorithm are used. Software elaborated on this basis is used for analysis of hysteresis loss in the core. Selected results of investigations are shown.

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MOLLAH, S. "THERMAL HYSTERESIS IN RESISTIVITY AND MAGNETIZATION OF PrCa(Sr)MnO." Modern Physics Letters B 22, no. 32 (December 30, 2008): 3241–48. http://dx.doi.org/10.1142/s021798490801762x.

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Thermal hysteresis in resistivity and magnetization of Pr 0.65 Ca 0.35-x Sr x MnO 3(x = 0–0.35) manganites has been systematically studied to establish the interplay of their charge and spin-ordering. The increasing Sr concentration (x) transforms the charge-ordered (CO)/antiferromagnetic (AFM) insulating system (for x = 0) into a mixed-phased one (for x = 0.1) with sharp metal–insulator (MI) transition and finally leads to a ferromagnetic (FM) metallic (for x = 0.35) system. It has been found that the interplay of charge and spin-ordering is higher in mixed-phased state and the thermal hysteresis loop area is bigger. It increases with the increase of sharpness of MI transition. Interplay of charge and spin-ordering decreases with the increase of either CO/AFM insulating or FM metallic phase and is almost absent in completely CO/AFM insulating (with x = 0) or FM metallic (with x = 0.35) states bringing about zero thermal hysteresis loop.

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