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Journal articles on the topic 'Heat Conduction'

Author: Grafiati

Published: 4 June 2021

Last updated: 31 July 2024

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1

Nath, Chandrani, A. Kumar, K. Z. Syu, and Y. K. Kuo. "Heat conduction in conducting polyaniline nanofibers." Applied Physics Letters 103, no. 12 (September 16, 2013): 121905. http://dx.doi.org/10.1063/1.4821656.

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2

Nujumdar, Arun S. "HEAT CONDUCTION." Drying Technology 7, no. 4 (December 1989): 837–38. http://dx.doi.org/10.1080/07373938908916634.

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3

Hammerschmidt, Ulf. "Heat Conduction." Thermochimica Acta 235, no. 1 (April 1994): 145–46. http://dx.doi.org/10.1016/0040-6031(94)80092-8.

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4

Heggs, P. J. "Heat conduction." Chemical Engineering Journal and the Biochemical Engineering Journal 55, no. 1-2 (August 1994): 98–99. http://dx.doi.org/10.1016/0923-0467(94)87020-9.

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5

Yovanovich, M. M. "Heat conduction." International Journal of Heat and Fluid Flow 6, no. 3 (September 1985): 192. http://dx.doi.org/10.1016/0142-727x(85)90009-8.

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6

Singham, J. R. "Heat conduction." International Journal of Heat and Fluid Flow 7, no. 1 (March 1986): 80. http://dx.doi.org/10.1016/0142-727x(86)90049-4.

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7

Beck, James V. "Heat conduction." International Journal of Heat and Fluid Flow 8, no. 1 (March 1987): 71. http://dx.doi.org/10.1016/0142-727x(87)90053-1.

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8

Ali, Y. M., and L. C. Zhang. "Relativistic heat conduction." International Journal of Heat and Mass Transfer 48, no. 12 (June 2005): 2397–406. http://dx.doi.org/10.1016/j.ijheatmasstransfer.2005.02.003.

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9

Votrubová, J., M. Dohnal, T. Vogel, and M. Tesař. "On parameterization of heat conduction in coupled soil water and heat flow modelling." Soil and Water Research 7, No. 4 (November 9, 2012): 125–37. http://dx.doi.org/10.17221/21/2012-swr.

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Soil water and heat transport plays an important role in various hydrologic, agricultural, and industrial applications. Accordingly, an increasing attention is paid to relevant simulation models. In the present study, soil thermal conditions at a mountain meadow during the vegetation season were simulated. A dual-continuum model of coupled water and heat transport was employed to account for preferential flow effects. Data collected at an experimental site in the &Scaron;umava Mountains, southern Bohemia, during the vegetation season 2009 were employed. Soil hydraulic properties (retention curve and hydraulic conductivity) determined by independent soil tests were used. Unavailable hydraulic parameters were adjusted to obtain satisfactory hydraulic model performance. Soil thermal properties were estimated based on values found in literature without further optimization. Three different approaches were used to approximate the soil thermal conductivity function, λ(θ): (i) relationships provided by Chung and Horton (ii) linear estimates as described by Loukili, Woodbury and Snelgrove, (iii) methodology proposed by Côté and Konrad. The simulated thermal conditions were compared to those observed. The impact of different soil thermal conductivity approximations on the heat transport simulation results was analysed. The differences between the simulation results in terms of the soil temperature were small. Regarding the surface soil heat flux, these differences became substantial. More realistic simulations were obtained using λ(θ) estimates based on the soil texture and composition. The differences between these two, related to neglecting vs. considering λ(θ) non-linearity, were found negligible.

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10

D’Alessandro, Giampaolo, and Filippo de Monte. "Multi-Layer Transient Heat Conduction Involving Perfectly-Conducting Solids." Energies 13, no. 24 (December 8, 2020): 6484. http://dx.doi.org/10.3390/en13246484.

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Boundary conditions of high kinds (fourth and sixth kind) as defined by Carslaw and Jaeger are used in this work to model the thermal behavior of perfect conductors when involved in multi-layer transient heat conduction problems. In detail, two- and three-layer configurations are analyzed. In the former, a thin layer modeled as a lumped body is subject to a surface heat flux on the front side while it is in perfect (fourth kind) or in imperfect (sixth kind) thermal contact with a semi-infinite or finite body on the back side. When dealing with a semi-infinite body in imperfect contact, the temperature solution is derived by means of the Laplace transform method. Green’s function approach is also used but for solving the companion case of a finite body in perfect contact with the thin film. In the latter, a thin layer with internal heat generation is located between two semi-infinite or finite bodies in perfect/imperfect contact. For the sake of thermal symmetry, such a three-layer structure reduces to a two-layer configuration. Results are given in both tabular and graphical forms and show the effect of heat capacity and thermal resistance on the temperature distribution of conductive layers.

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11

Szekeres, András, and Balázs Fekete. "Continuummechanics – Heat Conduction – Cognition." Periodica Polytechnica Mechanical Engineering 59, no. 1 (2015): 8–15. http://dx.doi.org/10.3311/ppme.7152.

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12

Kim, E. K., S. I. Kwun, S. M. Lee, H. Seo, and J. G. Yoon. "Heat conduction inZnS:SiO2composite films." Physical Review B 61, no. 9 (March 1, 2000): 6036–40. http://dx.doi.org/10.1103/physrevb.61.6036.

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13

Aebischer, Beat. "Heat Conduction in Lenses." Mathematical Problems in Engineering 2007 (2007): 1–28. http://dx.doi.org/10.1155/2007/57360.

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We consider several heat conduction problems for glass lenses with different boundary conditions. The problems dealt with in Sections sec:1 to sec:3 are motivated by the problem of an airborne digital camera that is initially too cold and must be heated up to reach the required image quality. The problem is how to distribute the heat to the different lenses in the system in order to reach acceptable operating conditions as quickly as possible. The problem of Section sec:4 concerns a space borne laser altimeter for planetary exploration. Will a coating used to absorb unwanted parts of the solar spectrum lead to unacceptable heating? In this paper, we present analytic solutions for idealized cases that help in understanding the essence of the problems qualitatively and quantitatively, without having to resort to finite element computations. The use of dimensionless quantities greatly simplifies the picture by reducing the number of relevant parameters. The methods used are classical: elementary real analysis and special functions. However, the boundary conditions dictated by our applications are not usually considered in classical works on the heat equation, so that the analytic solutions given here seem to be new. We will also show how energy conservation leads to interesting sum formulae in connection with Bessel functions. The other side of the story, to determine the deterioration of image quality by given (inhomogeneous) temperature distributions in the optical system, is not dealt with here.

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14

Hondzo, Midhat, and Heinz G. Stefan. "Riverbed heat conduction prediction." Water Resources Research 30, no. 5 (May 1994): 1503–13. http://dx.doi.org/10.1029/93wr03508.

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15

Alassar, R. S. "Heat Conduction From Spheroids." Journal of Heat Transfer 121, no. 2 (May 1, 1999): 497–99. http://dx.doi.org/10.1115/1.2826010.

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16

Khvesyuk, V. I., and A. S. Skryabin. "Heat conduction in nanostructures." High Temperature 55, no. 3 (May 2017): 434–56. http://dx.doi.org/10.1134/s0018151x17030129.

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17

Wang, Liqiu, and Xiaohao Wei. "Heat conduction in nanofluids." Chaos, Solitons & Fractals 39, no. 5 (March 2009): 2211–15. http://dx.doi.org/10.1016/j.chaos.2007.06.072.

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18

Hui, Ping. "Integrals from Heat Conduction." SIAM Review 38, no. 4 (December 1996): 668–69. http://dx.doi.org/10.1137/1038122.

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19

Taillefer, Louis, Benoit Lussier, Robert Gagnon, Kamran Behnia, and Hervé Aubin. "Universal Heat Conduction inYBa2Cu3O6.9." Physical Review Letters 79, no. 3 (July 21, 1997): 483–86. http://dx.doi.org/10.1103/physrevlett.79.483.

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20

Abu-Jaradeh, Nafiz, and David L. Powers. "Heat conduction on graphs." Discrete Applied Mathematics 52, no. 1 (July 1994): 1–16. http://dx.doi.org/10.1016/0166-218x(92)00183-m.

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21

Franceschini, Chiara, Rouven Frassek, and Cristian Giardinà. "Integrable heat conduction model." Journal of Mathematical Physics 64, no. 4 (April 1, 2023): 043304. http://dx.doi.org/10.1063/5.0138013.

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We consider a stochastic process of heat conduction where energy is redistributed along a chain between nearest neighbor sites via an improper beta distribution. Similar to the well-known Kipnis–Marchioro–Presutti (KMP) model, the finite chain is coupled at its ends with two reservoirs that break the conservation of energy when working at different temperatures. At variance with KMP, the model considered here is integrable, and one can write in a closed form the n-point correlation functions of the non-equilibrium steady state. As a consequence of the exact solution one, can directly prove that the system is in “local equilibrium,” which is described at the macro-scale by a product measure. Integrability manifests itself through the description of the model via the open Heisenberg chain with non-compact spins. The algebraic formulation of the model allows us to interpret its duality relation with a purely absorbing particle system as a change of representation.

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22

Brody, Jed, and Max Brown. "Transient heat conduction in a heat fin." American Journal of Physics 85, no. 8 (August 2017): 582–86. http://dx.doi.org/10.1119/1.4983649.

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23

Kovács, R., and P. Ván. "Generalized heat conduction in heat pulse experiments." International Journal of Heat and Mass Transfer 83 (April 2015): 613–20. http://dx.doi.org/10.1016/j.ijheatmasstransfer.2014.12.045.

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24

Li, Shu-Nan, and Bing-Yang Cao. "Lorentz covariance of heat conduction laws and a Lorentz-covariant heat conduction model." Applied Mathematical Modelling 40, no. 9-10 (May 2016): 5532–41. http://dx.doi.org/10.1016/j.apm.2016.01.007.

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25

Li, Wen Bo, Yin Gai Jin, Shuang Yin, and Pei Yan Chen. "Electrical Simulation Experiment and the Analysis of Thermal Conductivity of Materials." Advanced Materials Research 989-994 (July 2014): 599–602. http://dx.doi.org/10.4028/www.scientific.net/amr.989-994.599.

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s: Jilin university innovation experiment Electrical Simulation Experiment and the Analysis of Thermal Conductivity of Materials aims to solve the problem of thermocouple measuring tenderness in error. Thermocouple is used to measure temperature when measuring unsteady heat conduction in laboratory. The improved measuring method of unsteady heat conduction puts the breakthrough on the electric simulation method. The text bench is constructed by different shapes of conductive plate which is made of the graphite conductive paint, and voltmeter is refitted by diodes and controlled transformer. Through the test bench, we finished the simulation of unsteady heat conduction under the similar thermal conductive boundary conditions. Finally, the error analysis of experiment and the advantages of electric simulation method are given in this paper.

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26

Sheladiya, Manojkumar, Vinay Bhatt, Pratik Kikani, Sagarkumar Shah, and Jinesh Shah. "Research on Unsteady State Heat Conduction in Slab & Cylinder." Indian Journal of Applied Research 3, no. 8 (October 1, 2011): 250–52. http://dx.doi.org/10.15373/2249555x/aug2013/80.

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27

Hou, Fangxin, Xiang Zhang, Teng Hu, and Huajian Chang. "ICONE23-1360 A NEW DETERMINATION APPROACH ON CRITICAL HEAT FLUX WITH INVERSE HEAT CONDUCTION PROBLEM." Proceedings of the International Conference on Nuclear Engineering (ICONE) 2015.23 (2015): _ICONE23–1—_ICONE23–1. http://dx.doi.org/10.1299/jsmeicone.2015.23._icone23-1_168.

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28

Lv, Hong Yu, and Xue Xun Bian. "Analysis of Heat Dissipation and the Energy Conservation in Cast Iron Dryer Head of Paper Machine." Advanced Materials Research 503-504 (April 2012): 293–96. http://dx.doi.org/10.4028/www.scientific.net/amr.503-504.293.

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Analyzed the result computed of finite element heat transfer, discovered the temperature difference between the two sides of head is very small. Therefore its hot loss is very big. In addition, the temperature of dryer head flank is basically the same. Therefore the dryer head's heat dissipation can be simplified as a question of univariate heat conduction, also simplified to be a big plate heat conduction problem. This article offers simple algorithmic analysis of dryer head temperature field algorithm and the heat dissipation computation, and studied the head temperature computation and the heat dissipation analysis with a heat preservation board added. The importance that increased heat preservation board for energy conservation is pointed out.

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29

Jin, Junjie, Peiyao Duan, Yu Liu, Honglin Chen, and Tingting Yu. "Experimental Study on Convection and Heat Conduction Heating of an Air-Conditioned Bed System under Winter Lunch Break Mode." Processes 11, no. 8 (August 9, 2023): 2391. http://dx.doi.org/10.3390/pr11082391.

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In this paper, an experimental study of a system for heating an air-conditioned bed during a 2 h lunch was carried out. The results show that the power consumption of heat conduction heating was only 0.34 kW·h and that the average heat dissipation was 81.3 W, while the power consumption of convection heating was 1.43 kW·h, accompanied by an average heat dissipation of 748.7 W. Regardless of the power consumption or the heat dissipation, the convection heating was significantly higher than the heat conduction heating. As a result, the room air temperature increased from 12.3 °C to 17.3 °C under convection heating, but only increased from 14.4 °C to 15.2 °C under heat conduction heating. The study results indicate that when using heat conduction heating, water temperatures in the range of 38~40 °C could meet the thermal comfort needs of the human body; however, a higher temperature range was required when using convection heating. In contrast, the grade of the hot water required for heat conduction heating was lower. It was also found that the temperature under convection heating rises faster, but it tends to lead to a dry feeling after a long time, while the conductive heating showed a slower temperature rise. There was a cool feeling for 20 min when the heating started, and then the thermal comfort improved. The air-conditioning system in this paper was investigated in a heating experiment in the winter lunch break mode and compared with convection heating. The heat conduction heating resulted in better thermal comfort and higher energy efficiency. It is suggested to adopt the heat conduction heating mode in the winter heating operation of this system.

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30

Ibragimov, Nail H., and Elena D. Avdonina. "Heat Conduction in Anisotropic Media." Interdisciplinary journal of Discontinuity, Nonlinearity, and Complexity 1, no. 3 (September 2012): 237–51. http://dx.doi.org/10.5890/dnc.2012.06.002.

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31

Nishikawa, Seiki, Mohan Ramachandran, and Philippe Tondeur. "Heat conduction for Riemannian foliations." Bulletin of the American Mathematical Society 21, no. 2 (October 1, 1989): 265–68. http://dx.doi.org/10.1090/s0273-0979-1989-15826-6.

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32

Lesnic, D. "Heat conduction with mixed derivatives." International Journal of Computer Mathematics 81, no. 8 (August 2004): 971–77. http://dx.doi.org/10.1080/00207160410001715294.

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33

Krasheninnikov, S. I. "On nonlocal electron heat conduction." Physics of Fluids B: Plasma Physics 5, no. 1 (January 1993): 74–76. http://dx.doi.org/10.1063/1.860869.

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34

Morelli, D. T., J. Heremans, M. Sakamoto, and C. Uher. "Anisotropic Heat Conduction in Diacetylenes." Physical Review Letters 57, no. 7 (August 18, 1986): 869–72. http://dx.doi.org/10.1103/physrevlett.57.869.

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35

Baker-Jarvis, J., and R. Inguva. "Heat Conduction in Heterogeneous Materials." Journal of Heat Transfer 107, no. 1 (February 1, 1985): 39–43. http://dx.doi.org/10.1115/1.3247399.

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A new solution to the heat equation in composite media is derived using a variational principle developed by Ben-Amoz. The model microstructure is fed into the equations via a term for the polar moment of the inclusions in a representative volume. The general solution is presented as an integral in terms of sources and a Green function. The problem of uniqueness is studied to determine appropriate boundary conditions. The solution reduces to the solution of the normal heat equation in the limit of homogeneous media.

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36

Bobisud, L. E., and Tae s. Do. "A nonlocal heat conduction problem." Applicable Analysis 62, no. 3-4 (November 1996): 381–89. http://dx.doi.org/10.1080/00036819608840490.

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37

Wadsö, Lars. "Unthermostated Multichannel Heat Conduction Calorimeter." Cement, Concrete, and Aggregates 26, no. 2 (2004): 1–7. http://dx.doi.org/10.1520/cca12313.

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38

Alassar, Rajai, Mohammed Abushosha, and Mohammed El-Gebeily. "TRANSIENT HEAT CONDUCTION FROM SPHEROIDS." Transactions of the Canadian Society for Mechanical Engineering 38, no. 3 (September 2014): 373–89. http://dx.doi.org/10.1139/tcsme-2014-0027.

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We study the unsteady heat conduction from a spheroid (prolate or oblate) initially heated and then left to cool in an unbounded medium of constant temperature. We present two solutions of the problem. The first makes use of the spheroidal wave functions as basis. The second, which is numerical, is obtained by expanding the dimensionless temperature in terms of Legendre functions and then solving the resulting set of differential equations in the radial direction using an implicit finite difference scheme. The two solutions are further verified by comparing them to the limiting case of a sphere. We study the effect of the axis ratio on the time development of temperature inside the spheroid and the heat flux across the surface.

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39

Khvesyuk, V. I. "Heat conduction in multilayer nanostructures." Technical Physics Letters 42, no. 10 (October 2016): 985–87. http://dx.doi.org/10.1134/s1063785016100084.

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40

Chen, Gang. "Ballistic-Diffusive Heat-Conduction Equations." Physical Review Letters 86, no. 11 (March 12, 2001): 2297–300. http://dx.doi.org/10.1103/physrevlett.86.2297.

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41

Nettleton, R. E. "Nonlinear heat conduction in gases." Physical Review E 54, no. 2 (August 1, 1996): 2147–49. http://dx.doi.org/10.1103/physreve.54.2147.

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42

Chen, Gang. "Phonon heat conduction in nanostructures." International Journal of Thermal Sciences 39, no. 4 (April 2000): 471–80. http://dx.doi.org/10.1016/s1290-0729(00)00202-7.

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43

Boutin, C. "Microstructural influence on heat conduction." International Journal of Heat and Mass Transfer 38, no. 17 (November 1995): 3181–95. http://dx.doi.org/10.1016/0017-9310(95)00072-h.

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44

Tachoire, H., and V. Torra. "Thermokinetics by heat-conduction calorimetry." Thermochimica Acta 110 (February 1987): 171–81. http://dx.doi.org/10.1016/0040-6031(87)88225-4.

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45

Collet, P., and J. P. Eckmann. "A Model of Heat Conduction." Communications in Mathematical Physics 287, no. 3 (November 21, 2008): 1015–38. http://dx.doi.org/10.1007/s00220-008-0691-2.

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46

Luckyanova, M. N., J. Mendoza, H. Lu, B. Song, S. Huang, J. Zhou, M. Li, et al. "Phonon localization in heat conduction." Science Advances 4, no. 12 (December 2018): eaat9460. http://dx.doi.org/10.1126/sciadv.aat9460.

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Nondiffusive phonon thermal transport, extensively observed in nanostructures, has largely been attributed to classical size effects, ignoring the wave nature of phonons. We report localization behavior in phonon heat conduction due to multiple scattering and interference events of broadband phonons, by measuring the thermal conductivities of GaAs/AlAs superlattices with ErAs nanodots randomly distributed at the interfaces. With an increasing number of superlattice periods, the measured thermal conductivities near room temperature increased and eventually saturated, indicating a transition from ballistic to diffusive transport. In contrast, at cryogenic temperatures the thermal conductivities first increased but then decreased, signaling phonon wave localization, as supported by atomistic Greenșs function simulations. The discovery of phonon localization suggests a new path forward for engineering phonon thermal transport.

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47

Vadasz, Peter. "Heat Conduction in Nanofluid Suspensions." Journal of Heat Transfer 128, no. 5 (October 7, 2005): 465–77. http://dx.doi.org/10.1115/1.2175149.

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The heat conduction mechanism in nanofluid suspensions is derived for transient processes attempting to explain experimental results, which reveal an impressive heat transfer enhancement. In particular, the effect of the surface-area-to-volume ratio (specific area) of the suspended nanoparticles on the heat transfer mechanism is explicitly accounted for, and reveals its contribution to the specific solution and results. The present analysis might provide an explanation that settles an apparent conflict between the recent experimental results in nanofluid suspensions and classical theories for estimating the effective thermal conductivity of suspensions that go back more than one century (Maxwell, J.C., 1891, Treatise on Electricity and Magnetism). Nevertheless, other possible explanations have to be accounted for and investigated in more detail prior to reaching a final conclusion on the former explanation.

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48

Atkinson, C. "Heat conduction within linear thermoelasticity." International Journal of Heat and Mass Transfer 29, no. 10 (October 1986): 1611. http://dx.doi.org/10.1016/0017-9310(86)90078-5.

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49

Yuen, W. Y. D. "Heat conduction in sliding solids." International Journal of Heat and Mass Transfer 31, no. 3 (March 1988): 637–46. http://dx.doi.org/10.1016/0017-9310(88)90045-2.

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50

Klamkin, M. S. "An anomalous heat conduction problem." Mathematical and Computer Modelling 12, no. 6 (1989): 671–72. http://dx.doi.org/10.1016/0895-7177(89)90353-1.

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