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Number of results: 28
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Abstract

In this study the results of simultaneous measurements of dynamic viscosity, thermal conductivity, electrical conductivity and pH of two nanofluids, i.e., thermal oil/Al2O3and thermal oil/TiO2are presented. Thermal oil is selected as a base liquid because of possible application in ORC systems as an intermediate heating agent. Nanoparticles were tested at the concentration of 0.1%, 1%, and 5% by weight within temperature range from 20°C to 60°C. Measurement devices were carefully calibrated by comparison obtained results for pure base liquid (thermal oil) with manufacturer’s data. The results obtained for tested nanofluids were compared with predictions made by use of existing models for liquid/solid particles mixtures.
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Authors and Affiliations

Janusz T. Cieśliński
Katarzyna Ronewicz
Sławomir Smoleń
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Abstract

Nonlinear excitation of the entropy perturbations by magnetosonic waves in a uniform and infinite plasma model is considered. The wave vector of slow or fast mode forms an arbitrary angle θ (0≤θ≤π) with the equilibrium straight magnetic field, and all perturbations are functions of the time and longitudinal coordinate. Thermal conduction is the only factor which destroys isentropicity of wave perturbations and causes the nonlinear excitation of the entropy mode. A dynamic equation is derived which describes excitation of perturbation in the entropy mode in the field of dominant magnetosonic mode. Effects associatiated with temperature dependent and anisotropic thermal conduction are considered and discussed.
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Bibliography

1. Afanasyev A.N., Nakariakov V.M. (2014), Nonlinear slow magnetoacoustic waves in coronal plasma structures, Astronomy and Astrophysics, 573: A32, doi: 10.1051/0004-6361/201424516.
2. Ballai I. (2006), Nonlinear waves in solar plasmas – a review, Journal of Physics: Conference Series, 44(20): 20–29, doi: 10.1088/1742-6596/44/1/003.
3. Braginskii S.I. (1965), Transport processes in plasma, Reviews of Plasma Physics, M.A. Leontovich [Ed.], Vol. 1, p. 205, Consultants Bureau, New York.
4. Callen J.D. (2003), Fundamentals of Plasma Physics, Lecture Notes, University of Wisconsin, Madison.
5. Chin R., Verwichte E., Rowlands G., Nakariakov V.M. (2010), Self-organization of magnetoacoustic waves in a thermal unstable environment, Physics of Plasmas, 17(32): 107–118, doi: 10.1063/1.3314721.
6. Dahlburg R.B., Mariska J.T. (1988), Influence of heating rate on the condensational instability, Solar Physics, 117(1): 51–56, doi: 10.1007/BF00148571.
7. Field G.B. (1965), Thermal instability, The Astrophysical Journal, 142: 531–567, doi: 10.1086/148317.
8. Heyvaerts J. (1974), The thermal instability in a magnetohydrodynamic medium, Astronomy and Astrophysics, 37(1): 65–73.
9. Hollweg J.V. (1985), Viscosity in a magnetized plasma: Physical interpretation, Journal of Geophysical Research, 90(A8): 7620–7622, doi: 10.1029/JA090iA08p07620.
10. Ibáñez S.M.H., Parravano A. (1994), On the thermal structure and stability of configurations with heat diffusion and a gain-loss function. 3: Molecular gas, The Astrophysical Journal, 424(2): 763–771, doi: 10.1086/173929.
11. Krall N.A., Trivelpiece A.W. (1973), Principles of Plasma Physics, McGraw Hill, New York.
12. Kumar N., Kumar P., Singh S. (2006), Coronal heating by MHD waves, Astronomy and Astrophysics, 453: 1067–1078, doi: 10.1051/0004-6361:20054141.
13. Leble S., Perelomova A. (2018), The Dynamical Projectors Method: Hydro and Electrodynamics, CRC Press.
14. De Moortel I., Hood A.W. (2004), The damping of slow MHD waves in solar coronal magnetic fields, Astronomy and Astrophysics, 415: 705–715, doi: 10.1051/0004-6361:20034233.
15. Nakariakov V.M., Mendoza-Briceño C.A., Ibáñez M.H. (2000), Magnetoacoustic waves of small amplitude in optically thin quasi-isentropic plasmas, The Astrophysical Journal, 528(2, Part 1): 767–775, doi: 10.1086/308195.
16. Ofman L., Wang T. (2002), Hot coronal loop oscillations observed by SUMER: slow magnetosonic wave damping by thermal conduction, The Astrophysical Journal, 580(1): L85–L88, doi: 10.1086/345548.
17. Parker E.N. (1953), Instability of thermal fields, The Astrophysical Journal, 117: 431–436, doi: 10.1086/145707.
18. Perelomova A. (2006), Development of linear projecting in studies of non-linear flow. Acoustic heating induced by non-periodic sound, Physics Letters A, 357: 42–47, doi: 10.1016/j.physleta.2006.04.014.
19. Perelomova A. (2008), Modelling of acoustic heating induced by different types of sound, Archives of Acoustics, 33(2): 151–160.
20. Perelomova A. (2018a), Magnetoacoustic heating in a quasi-isentropic magnetic gas, Physics of Plasmas, 25: 042116, doi: 10.1063/1.5025030.
21. Perelomova A. (2018b), Magnetoacoustic heating in nonisentropic plasma caused by different kinds of heating-cooling function, Advances in Mathematical Physics, 2018: Article ID 8253210, 12 pages, doi: 10.1155/2018/8253210.
22. Perelomova A. (2020), Hysteresis curves for some periodic and aperiodic perturbations in magnetosonic flow, Physics of Plasmas, 27(10): 102101, doi: 10.1063/5.0015944.
23. Ruderman M.S., Verwichte E., Erdélyi R., Goossens M. (1996), Dissipative instability of the MHD tangential discontinuity in magnetized plasmas with an isotropic viscosity and thermal conductivity, Journal of Plasma Physics, 56(2): 285–306, doi: 10.1017/S0022377800019279.
24. Sabri S., Poedts S., Ebadi H. (2019), Plasma heating by magnetoacoustic wave propagation in the vicinity of a 2.5D magnetic null-point, Astronomy and Astrophysics, 623, doi: 10.1051/0004-6361/201834286.
25. Soler R., Ballester J.L., Parenti S. (2012), Stability of thermal modes in cool prominence plasmas, Astronomy and Astrophysics, 540: A7, doi: 10.1051/0004-6361/201118492.
26. Spitzer L. (1962), Physics of Fully Ionized Gases, 2nd ed., New York, Interscience.
27. Vesecky J.F., Antiochos S.K., Underwood J.H. (1979), Numerical modeling of quasi-static coronal loops. I – Uniform energy input, The Astrophysical Journal, 233(3): 987–997, doi: 10.1086/157462.
28. Wang T. (2011), Standing slow-mode waves in hot coronal loops: observations, modeling, and coronal seismology, Space Science Reviews, 158: 397–419, doi: 10.1007/s11214-010-9716-1.
29. Zavershinskii D.I., Molevich N.E., Riashchikov D.S., Belov S.A. (2020), Nonlinear magnetoacoustic waves in plasma with isentropic thermal instability, Physical Review E, 101(4): 043204, doi: 10.1103/PhysRevE.101.043204.
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Authors and Affiliations

Anna Perelomova
1

  1. Gdansk University of Technology, Faculty of Applied Physics and Mathematics, Gdansk, Poland
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Abstract

This paper investigates the thermal and mechanical properties of a composite made from a combination of 2063-epoxy resin and three different braided carbon-fiber fabric reinforcements. These fibres consist of HTS carbon, HTS carbon braided with nickel coated carbon and HTS carbon braided with nickel coated copper, respectively. The composites were manufactured through resin transfer molding (RTM) route. The thermal diffusivity of carbon fibers composites was measured at different temperature by using a flash method. The transverse and planar thermal conductivities were determined by measuring the specific heat, density and thermal diffusivities, respectively. The current research highlights the influence of adding nickel coated carbon and nickel-plated copper wires on the braided composites. The evaluation shows that the HTS carbon braided manufactured with nickel-plated copper wires presents higher in-plane thermal conductivity (in direction parallel of the fibres) when comparing to HTS carbon and HTS carbon braided manufactured with nickel coated carbon. The thermal conductivity benefits of those composite were achieved at the expenses of lower mechanical properties of braided composites investigated.
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Authors and Affiliations

Jamal Arbaoui
1 2
ORCID: ORCID
Jérémie Aucher
1
ORCID: ORCID
Moussa Gomina
1
ORCID: ORCID
Joel Breard
1
ORCID: ORCID

  1. Laboratoire CRISMAT, UMR 6508 CNRS/ENSICAEN, 6 Bd Maréchal Juin, 14050 Caen Cedex 4, France
  2. University of Cadi Ayyad, National School of Applied Sciences, Laboratory of Materials, Processes, Environment and Quality, B.P. 63, 46000, Safi, Morocco
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Abstract

Reliable knowledge of thermo-physical properties of materials is essential for the interpretation of solidification behaviour, forming, heat treatment and joining of metallic systems. It is also a precondition for precise simulation calculations of technological processes. Numerical calculations usually require the knowledge of temperature dependencies of three basic thermo-physical properties: thermal conductivity, heat capacity and density. The objective of this work is to find a correlation that fits the thermal conductivity of selected steel grades as a function of temperature (within the range of 0–800°C) and carbon content (within the range of 0.1–0.6%). The starting point for the analysis are the experimental data on thermal conductivity taken from literature. Using the method of least squares it was possible to fit an equation which allows calculating the thermal conductivity of steel depending on the temperature and carbon content. Two kinds of equations have been analyzed: a linear one (a linear model) and a second degree polynomial (a non-linear model). The thermal conductivity obtained by linear and nonlinear models varies on average from the measured values by 3% and 2.6% respectively.
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Authors and Affiliations

Rafał Wyczółkowski
1
Dominika Strychalska
1
Vazgen Bagdasaryan
2

  1. Czestochowa University of Technology, Department of Production Management, Armii Krajowej 19, 42-200 Czestochowa, Poland
  2. Warsaw University of Life Sciences, Institute of Civil Engineering – SGGW, Nowoursynowska 166, 02-787 Warsaw, Poland
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Abstract

Main goal of the paper is to present the algorithm serving to solve the heat conduction inverse problem. Authors consider the heat conduction equation with the Riemann-Liouville fractional derivative and with the second and third kind boundary conditions. This type of model with fractional derivative can be used for modelling the heat conduction in porous media. Authors deal with the heat conduction inverse problem, which, in this case, consists in identifying an unknown thermal conductivity coefficient. Measurements of temperature, in selected point of the region, are the input data for investigated inverse problem. Basing on this information, a functional describing the error of approximate solution is created. Minimizing of this functional is necessary to solve the inverse problem. In the presented approach the Ant Colony Optimization (ACO) algorithm is used for minimization.

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Authors and Affiliations

R. Brociek
D. Słota
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Abstract

In this study, agar-based nanocomposite films containing ultra-porous silica aerogel particles were fabricated by gel casting using an aqueous agar/silica aerogel slurry. The silica aerogel particles did not show significant agglomeration and were homogeneously distributed in the agar matrix. Transmission electron microscopy observations demonstrated that the silica aerogel particles had a mesoporous microstructure and their pores were not incorporated into the agar polymer molecules. The thermal conductivities of the agar and agar/5 wt.% silica aerogel nanocomposite films were 0.36 and 0.20 W·m–1·K–1, respectively. The transmittance of the agar films did not decrease upon the addition of silica aerogel particles into them. This can be attributed to the anti-reflection effect of silica aerogel particles.

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Authors and Affiliations

Min-Jin Lee
Hyun-Ah Jung
Kyong-Jin Lee
Haejin Hwang
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Abstract

The article presents the prototype of a measurement system with a hot probe, designed for testing thermal parameters of heat insulation materials. The idea is to determine parameters of thermal insulation materials using a hot probe with an auxiliary thermometer and a trained artificial neural network. The network is trained on data extracted from a nonstationary two-dimensional model of heat conduction inside a sample of material with the hot probe and the auxiliary thermometer. The significant heat capacity of the probe handle is taken into account in the model. The finite element method (FEM) is applied to solve the system of partial differential equations describing the model. An artificial neural network (ANN) is used to estimate coefficients of the inverse heat conduction problem for a solid. The network determines values of the effective thermal conductivity and effective thermal diffusivity on the basis of temperature responses of the hot probe and the auxiliary thermometer. All calculations, like FEM, training and testing processes, were conducted in the MATLAB environment. Experimental results are also presented. The proposed measurement system for parameter testing is suitable for temporary measurements in a building site or factory.

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Authors and Affiliations

Stanisław Chudzik
Waldemar Minkina
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Abstract

The article presents a novel method that allows measurement of thermal conductivity that is based on Stefan-Boltzmann law. The developed method can be used to determine thermal conductivity of ceramic investment casting molds. The methodology for conducting thermal conductivity tests of ceramic material samples is presented. Knowledge of the value of thermal capacity and thermal conductivity as a function of temperature enables computer simulations of the process of cooling and solidification of liquid metal in a mold.

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Authors and Affiliations

W. Leśniewski
E. Czekaj
P. Wieliczko
M. Wawrylak
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Abstract

In the present article, we introduced a new model of the equations of general ized thermoelasticity for unbounded orthotropic body containing a cylindrical cavity. We applied this model in the context of generalized thermoelasticity with phase-lags under the effect of rotation. In this case, the thermal conductivity of the material is considered to be variable. In addition, the cylinder surface is traction free and subjected to a uniform unit step temperature. Using the Laplace transform technique, the distributions of the temperature, displacement, radial stress and hoop stress are determined. A detailed analysis of the effects of rotation, phase-lags and the variability thermal conductivity parameters on the studied fields is discussed. Numerical results for the studied fields are illustrated graphically in the presence and absence of rotation.

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Authors and Affiliations

D.S. Mashat
Ashraf M. Zenkour
A.E. Abouelregal
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Abstract

By simulating the actual working conditions of a cable, the temperature variation rule of different measuring points under different load currents was analyzed. On this basis, a three-dimensional finite element model (FEM) was established, and the difference and influence factors between the simulation temperature and the experimental measured value were discussed, then the influence of thermal conductivity on the operating temperature of the conductor layer was studied. Finally, combined with the steady-state thermal conductivity model and the experimental measured data, the relation between thermal conductivity and load current was obtained.

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Authors and Affiliations

Xiaokai Meng
Peijie Han
Yongxin Liu
Zhumao Lu
Tao Jin
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Abstract

In this study, the thermal conductivity ratio model for metallic oxide based nano-fluids is proposed. The model was developed by considering the thermal conductivity as a function of particle concentration (percentage volume), temperature, particle size and thermal conductivity of the base fluid and nano-particles. The experimental results for Al2O3, CuO, ZnO, and TiO2 particles dispersed in ethylene glycol, water and a combination of both were adopted from the literature. Artificial neural network (ANN) and power law models were developed and compared with the experimental data based on statistical methods. ANOVA was used to determine the relative importance of contributing factors, which revealed that the concentration of nano-particles in a fluid is the single most important contributing factor of the conductivity ratio.
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Authors and Affiliations

Mohammad Hanief
1
Qureshi Irfan
1
Malik Parvez
2

  1. Mechanical Engineering Department, National Institute of Technology Srinagar, India
  2. Chemical Engineering Department, National Institute of Technology Srinagar, India
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Abstract

The influence of nano dispersion on the thermoelectric properties of Bi2Te3 was actively investigating to wide-spread thermoelectric applications. Herein this report, we have systematically controlled the microstructure of Bi0.5Sb1.5Te3 (BST) alloys through the incorporation of carbon nanofiber (CNF), and studied their effect on thermoelectric properties, and mechanical properties. The BST/x-CNF (x-0, 0.05, 0.1, 0.2 wt.%) composites powder was fabricated using high energy ball milling, and subsequently consolidated the powder using spark plasma sintering. The identification of CNF in bulk composites was analyzed in Raman spectroscopy and corresponding CNF peaks were recognized. The BST matrix grain size was greatly reduced with CNF dispersion and consistently decreased along CNF percentage. The electrical conductivity was reduced and Seebeck coefficient varied in small-scale by embedding CNF. The thermal conductivity was progressively diminished, obtained lattice thermal conductivity was lowest compared to bare sample due to induced phonon scattering at interfaces of secondary phases as well as highly dense fine grain boundaries. The peak ZT of 0.95 achieved for 0.1 wt.% dispersed BST/CNF composites. The Vickers hardness value of 101.8 Hv was obtained for the BST/CNF composites.
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Bibliography

[1] J.R. Szczech, J.M. Higgins, S. Jin, Enhancement of the thermoelectric properties in nanoscale and nanostructured materials, J. Mater. Chem. 21 (12), 4037-4055 (2011).
[2] Y. Pei, X. Shi, A. Lalonde, H. Wang, L. Chen, G.J. Synder, Convergence of electronic bands for high performance bulk thermoelectrics, Nature 473, 66-69 (2011).
[3] R . Deng, X. Su, S. Hao, Z. Zheng, M. Zhang, H. Xoe, W. Liu, Y. Yan, C. Wolverton, C. Uher, M.G. Kanatzidis, X. Tang, High thermoelectric performance in Bi0.46Sb1.54Te3 nanostructured with ZnTe, Energy Environ. Sci. 11, 1520-1535 (2018).
[4] H . Mamur, M.R.A Bhuiyan, F. Korkmaz, M. Nil, A review on bismuth telluride (Bi2Te3) nanostructure for thermoelectric applications, Renew. Sust. Energ. Rev. 82, 4159-4169 (2018).
[5] I . Chowdhury, R. Prasher, K. Lofgreen, G. Chrysler, S. Narasimhan, R. Mahajan, R. Venkatasubramanian, On-chip cooling by superlattice-based thin-film thermoelectrics, Nat. Nanotechnol. 4 (4), 235-238 (2009).
[6] Z. Xiao, X. Zhu, On-Chip Sensing of Thermoelectric Thin Film’s Merit, Sensors 15 (7), 17232-17240 (2015).
[7] X. Hu, X. Fan, B. Feng, D. Kong, P. Liu, R. Li, Y. Zhang, G. Li, Y. Li, Microstructural refinement, and performance improvement of cast n-type Bi2Te2.79Se0.21 ingot by equal channel angular extrusion, Met. Mater. Int. (2020). DOI: https://doi.org/10.1007/s12540-020-00699-5
[8] M. Sabarinathan, M. Omprakash, S. Harish, M. Navaneethan, J. Archana, S. Ponnusamy, Y. Hayakawa, Enhancement of power factor by energy filtering effect in hierarchical BiSbTe3 nanostructures for thermoelectric applications, Appl. Surf. Sci. 418, 246-251 (2017).
[9] B . Madavali, H.S. Kim, K.H. Lee, S.J. Hong, Enhanced Seebeck coefficient by energy filtering in Bi-Sb-Te based composites with dispersed Y2O3 nanoparticles, Intermetallics 82, 68-75 (2017).
[10] J. Hu, B. Liu, H. Subramanyan, B. Li, J. Zhou, J. Liu, Enhanced thermoelectric properties through minority carriers blocking in nanocomposites, J. Appl. Phys. 126 (9), 095107 (2019).
[11] S. Foster, N. Neophytou, Effectiveness of nano inclusions for reducing bipolar effects in thermoelectric materials, Comput. Mater. Sci. 164, 91-98 (2019).
[12] L.D. Hicks, T.C. Harman, X. Sun, M.S. Dresselhaus, Experimental study of the effect of quantum-well structures on the thermoelectric figure of merit, Phys. Rev. B 53 (16), R10493-R10496 (1996).
[13] I .V. Zaporotskova, N.P. Boroznina, Y.N. Parkhomenko, L.V. Kozhitov, Carbon nanotubes: Sensor properties, A review, Mod. Electron. Mater. 2 (4), 95-105 (2016).
[14] P.A. Tran, L. Zhang, T.J. Webster, Carbon nanofibers and carbon nanotubes in regenerative medicine, Adv. Drug Deliv. Rev. 61 (12), 1097-1114 (2009).
[15] M. Gurbuz, T. Mutuk, P. Uyan, Mechanical, Wear and Thermal behaviors of graphene reinforced titanium composites, Met. Mater. Int. (2020). DOI: https://doi.org/10.1007/s12540-020-00673-1
[16] D.W. Jung, J.H. Jeong, B.C. Cha, J.B. Kim, B.S. Kong, J.K. Lee, E.S. Oh, Effects of ball-milled graphite in the synthesis of SnO2/graphite as an active material in lithium-ion batteries, Met. Mater. Int. 17 (6), 1021-1026 (2011).
[17] A comparison of Carbon Nanotubes and Carbon Nanofibers, Pyrograf products, Inc, An affiliate of Applied surface sciences, Inc.
[18] K.M. Nam, K. Mees, H.S. Park, M. Willert-Porada, C.S. Lee, Electrophoretic Deposition for the Growth of Carbon nanofibers on Ni-Cu/C-fiber Textiles, Bull. Korean Chem. Soc. 35 (8), 2431- 2437 (2014).
[19] S .J. Jung, S.Y. Park, B.K. Kim, B. Kwon, S.K. Kim, H.H. Park, S.H. Baek, Hardening of Bi-Te based alloys by dispersing B4C nanoparticles, Acta Mater. 97, 68-74 (2015).
[20] C. Marquez, N. Rodriguez, R. Ruiz, F. Gamiz, Electrical characterization and conductivity optimization of laser reduced graphene oxide on insulator using point-contact methods, RSC Adv. 6 (52), 46231-46237 (2016).
[21] P. Sharief, B. Madavali, J.M. Koo, H.J. Kim, S. Hong, S.J. Hong, Effect of milling time parameter on the microstructure and the thermoelectric properties of N-type Bi2Te2.7Se0.3 alloys, Arch. Metall. Mater. 2, 585-590 (2019).
[22] P . Slobodian, P. Riha, R. Olejnik, M. Kovar, P. Svoboda, Thermoelectric properties of carbon nanotube and nanofiber based ethylene-octene copolymer composites for thermoelectric devices, J. Nanomater 2013, 1-7 (2013).
[23] Q. Lognoné, F. Gascoin, On the effect of carbon nanotubes on the thermoelectric properties of n-Bi2Te2. 4Se0. 6 made by mechanical alloying, J. Alloys Compd. 635, 107-111 (2015).
[24] B. Feng, G. Li, X. Hu, P. Liu, R. Li, Y. Zhang, Z. He, Improvement of thermoelectric and mechanical properties of BiCuSeO-based materials by SiC nanodispersion, J. Alloys Compd. 818, 152899 (2020).
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Authors and Affiliations

P. Sharief
1
B. Madavali
1
Y. Sohn
2
J.H. Han
2
G. Song
1
S.H. Song
1
S.J. Song
1

  1. Kongju National University, Division of Advanced Materials Engineering & Institute for Rare Metals, Cheonan, 331-717, Republic of Korea
  2. Chungnam National University, Department of Materials Science & Engineering, Daejeon, 34134, Republic of Korea
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Abstract

In this study, thermal conductivity, mechanical properties, and thermal degradation of pumice-added epoxy materials were investigated. 2%, 4%, 6%, 8%, and 10% of pumice was added to the epoxy resin (EP) % by weight. Various types of analyses and tests were conducted to determine the thermal conductivity, mechanical properties, and thermal degradation of these epoxy materials. The tests and analyses proved that the addition of pumice leads to a decrease in the thermal conductivity coefficient and density of the pure EP material. It also increases the degree of hardness. The addition of pumice had a positive effect on mechanical properties. Compared to pure EP, it increased the tensile strength, Young’s modulus, bending strength, and flexural modulus. As a result of TGA analysis it was determined that with the incorporation of pumice into the EP, its decomposition rate progressed more slowly. At 800_C, the carbon residue improved as a result of the addition of pumice.
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Authors and Affiliations

İbrahim Kırbaş
1
ORCID: ORCID

  1. Burdur Mehmet Akif Ersoy University, Department of Electrical and Energy, 15100, Burdur, Turkey
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Abstract

Heat transport when two surfaces of solids come into contact is an important phenomenon in many metallurgical processes. Determining the boundary conditions of heat transfer allows to obtain the correct solutions of the heat conduction equation. The paper presents models for determining the heat transfer coefficient between steel materials in contact. Experimental tests were carried out to measure the temperature changes of the contacting samples made of steel S235 (1.0038) and steel 15HM (1.7335) under the pressure of 10, 15 and 20 MPa. There was a large temperature difference between the samples. The results of the experiment were compared with numerically calculated temperatures and the value of the heat transfer coefficient was determined at different pressure values depending on the time.
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Authors and Affiliations

A. Przyłucka-Bednarska
1
ORCID: ORCID
M. Rywotycki
1
ORCID: ORCID
K. Sołek
1
ORCID: ORCID
Z. Malinowski
1
ORCID: ORCID

  1. AGH University of Science And Technology, Faculty of Metals Engineering and Industrial Computer Science, Al. Mickiewicza 30, 30-059 Krakow, Poland
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Abstract

The paper provides an overview of selected scientific articles presenting research carried out in recent years on methods for producing autoclaved aerated concrete. Traditional technologies are briefly presented, together with innovative solutions for the production of low-density and ultra-lowdensity materials. In addition to the presentation of the manufacturing methods themselves, the results of research into the properties of the autoclaved aerated concrete obtained and their dependence on the technology used are also presented. A subjective selection and review of articles covering research into the thermal conductivity of concrete, the technological factors influencing them and the ways in which they can be shaped was also carried out. A significant number of the cited articles do not function in the world scientific circulation due to the language barrier (they are mainly in Ukrainian). In the meantime, they contain interesting research results which can inspire further research into the issues discussed concerning the production technology and the thermal and strength properties of autoclaved aerated concrete, with particular emphasis on lightweight and ultra-lightweight concrete.
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Authors and Affiliations

Yaroslav Yakymechko
1
ORCID: ORCID
Roman Jaskulski
2
ORCID: ORCID
Maciej Banach
2
ORCID: ORCID
Piotr Perłowski
2
ORCID: ORCID

  1. Lviv Polytechnic National University, Institute of Chemistry and Chemical Technologies, Bandera str. 13, Lviv, Ukraine
  2. Warsaw University of Technology, Faculty of Civil Engineering Mechanics and Petrochemistry, ul. Łukasiewicza 17, 09-400 Płock, Poland
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Abstract

The work presents results of research on the influence of micro materials on the thermal conductivity λ of gypsum. In the research, cellulose-based polymer and aerogel were used as the modifying micro materials. For the purpose of measuring the thermal conductivity, a non-stationary method was used based on the “hot wire method”. A very precise set of devices for measuring and recording the temperature of the heating wire was used. In the presented solution, a single measurement took only one minute. Measurements were recorded with the help of a computer measuring system, with a sampling time of 0.01s. During the 60-second-long test, 6000 measurements of the heating wire temperature were collected. A decrease of the thermal conductivity and density of hardened gypsum with added micro materials was observed due to modifications of the structure of the final product. Experimental values of the thermal conductivity of the gypsum specimens with the addition of polymer and aerogel were respectively over 23% and 6% lower than the non-modified gypsum specimen.

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Authors and Affiliations

Karol Prałat
ORCID: ORCID
Roman Jaskulski
ORCID: ORCID
Justyna Ciemnicka
Grzegorz Makomaski
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Abstract

In this study, we investigated the effect of Fe addition (0, 0.25, 0.50 and 0.75 wt.%) on the microstructure, mechanical properties and electrical conductivity of as-cast and as-extruded Al-RE alloys. As the Fe element increased by 0 and 0.75wt.%, the phase fraction increased to 5.05, 5.76, 7.14 and 7.38 %. The increased intermetallic compound increased the driving force for recrystallization and grain refinement. The electrical conductivity of Al-1.0 wt.%RE alloy with Fe addition decreased to 60.29, 60.15, 59.58 and 59.13 %IACS. With an increase in the Fe content from 0 to 0.75 wt.% the ultimate tensile strength (UTS) of the alloy increased from 74.3 to 77.5 MPa. As the mechanical properties increase compared to the reduction of the electrical conductivity due to Fe element addition, it is considered to be suitable for fields requiring high electrical conductivity and strength.

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Authors and Affiliations

Hyo-Sang Yoo
ORCID: ORCID
Yong-Ho Kim
ORCID: ORCID
Hyeon-Taek Son
ORCID: ORCID
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Abstract

Free convection is one of the heat transfer modes which occurs within the heat-treated bundles of steel rectangular section. A comprehensive study of this phenomenon is necessary for optimizing the heating process of this type of charge. The free convection intensity is represented by the Rayleigh number Ra. The value of this criterion depends on the following parameters: the mean section temperature, temperature difference within the section, kinematic coefficient of viscosity, volume expansion coefficient and the Prandtl number. The paper presents the analysis of the impact of these factors on free convection in steel rectangular sections. The starting point for this analysis were the results of experimental examinations. It was found that the highest intensity of this process occurs for the temperature of 100°C. This is mainly caused by changes in the temperature difference observed in the area of sections and changes in kinematic coefficient of viscosity of air. The increase in the value of the Rayleigh number criterion at the initial stage is attributable to changes in the parameter of temperature difference within the section. After exceeding 100°C, the main effect on convection is from changes in air viscosity. Thus, with further increase in temperature, the Rayleigh number starts to decline rapidly despite further rise in the difference in temperature.
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Authors and Affiliations

Rafał Wyczółkowski
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Abstract

Heat and mass transfer stretched flow of an incompressible, electrically conducting Jeffrey fluid has been studied numerically. Nanoparticles are suspended in the base fluid and it has many applications such as cooling of engines, thermal absorption systems, lubricants fuel cell, nanodrug delivery system and so on. Temperature dependent variable thermal conductivity with Rosseland approximation is taken into account and suction effect is employed in the boundary conditions. The governing partial differential equations are first transformed into set of ordinary differential equations using selected similarity transformations, which are then solved numerically using Runge-Kutta-Felhberg fourth-fifth order method along with shooting technique. The flow, heat and mass transfer characteristics with local Nusselt number for various physical parameters are presented graphically and a detailed discussion regarding the effect of flow parameters on velocity and temperature profiles are provided. It is found that, increase of variable thermal conductivity, radiation, Brownian motion and thermophoresis parameter increases the rate of heat transfer. Local Nusselt number has been computed for various parameters and it is observed that, in the presence of variable thermal conductivity and Rosseland approximation, heat transfer characteristics are higher as compared to the constant thermal conductivity and linear thermal radiation.

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Authors and Affiliations

M. Archana
B.J. Gireesha
M.M. Rashidi
B.C. Prasannakumara
R.S.R. Gorla
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Abstract

In this study, a new laser flash system was proposed for the determination of the thermal conductivity of brown coal, hard coal and anthracite. The main objective of the investigation was to determine the effect of coal rank, composition, physical structure and temperature on thermal conductivity. The solid fuels tested were medium conductors of heat whose determined thermal conductivities were in the range of 0.09 to 0.23 W/(m K) at room temperature. The thermal conductivity of the solid fuels tested typically increased with the rank of coal and the measurement temperature. The results of this study show that the physical structure of solid fuels and temperature have a dominant effect on the fuels' thermal conductivity.

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Authors and Affiliations

Monika Kosowska-Golachowska
Władysław Gajewski
Tomasz Musiał
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Abstract

The aim of this work is the development of Cu-Al2O3 composites of copper Cu-ETP matrix composite materials reinforced by 20 and 30

vol.% Al2O3 particles and study of some chosen physical properties. Squeeze casting technique of porous compacts with liquid copper

was applied at the pressure of 110 MPa. Introduction of alumina particles into copper matrix affected on the significant increase of

hardness and in the case of Cu-30 vol. % of alumina particles to 128 HBW. Electrical resistivity was strongly affected by the ceramic

alumina particles and addition of 20 vol. % of particles caused diminishing of electrical conductivity to 20 S/m (34.5% IACS). Thermal

conductivity tests were performed applying two methods and it was ascertained that this parameter strongly depends on the ceramic

particles content, diminishing it to 100 Wm-1K-1 for the composite material containing 30 vol.% of ceramic particles comparing to 400

Wm-1K-1 for the unreinforced copper. Microstructural analysis was carried out using SEM microscopy and indicates that Al2O3 particles

are homogeneously distributed in the copper matrix. EDS analysis shows remains of silicon on the surface of ceramic particles after

binding agent used during preparation of ceramic preforms.

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Authors and Affiliations

J.W. Kaczmar
K. Granat
A. Kurzawa
E. Grodzka

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