Effect of temperature and composition on the volumetric, acoustic and thermal properties of N,N-dimethylformamide + propan-1-ol mixture

2019 ◽  
Vol 290 ◽  
pp. 111124 ◽  
Author(s):  
Magdalena Tyczyńska ◽  
Małgorzata Jóźwiak ◽  
Marlena Komudzińska ◽  
Tomasz Majak
2020 ◽  
Vol 32 (8) ◽  
pp. 04020210 ◽  
Author(s):  
Venkatesh Kodur ◽  
Srishti Banerji ◽  
Roya Solhmirzaei

1977 ◽  
Vol 20 (3) ◽  
pp. 0461-0464 ◽  
Author(s):  
E. B. Moysey ◽  
J. T. Shaw ◽  
W. P. Lampman

Author(s):  
John G. Michopoulos ◽  
Andrew Birnbaum ◽  
Athanasios P. Iliopoulos

Despite significant efforts examining the suitability of the proper form of the heat transfer partial differential equation (PDE) as a function of the time scale of interest (e.g. seconds, picoseconds, femtoseconds, etc.), very little work has been done to investigate the millisecond-microsecond regime. This paper examines the differences between the parabolic and one of the hyber-bolic forms of the heat conduction PDE that govern the thermal energy conservation on these intermediate timescales. Emphasis is given to the types of problems where relatively fast heat flux deposition is realized. Specifically, the classical parabolic form is contrasted against the lesser known Cattaneo-Vernotte hyperbolic form. A comparative study of the behavior of these forms over various pulsed conditions are applied at the center of a rectangular plate. Further emphasis is given to the variability of the solutions subject to constant or temperature-dependent thermal properties. Additionally, two materials, Al-6061 and refractory Nb1Zr, with widely varying thermal properties, were investigated.


2015 ◽  
Vol 31 (3) ◽  
pp. 1327-1330 ◽  
Author(s):  
Neetu Sorot ◽  
B. R. K Gupta

2015 ◽  
Vol 622 ◽  
pp. 777-782 ◽  
Author(s):  
Jie Su ◽  
Zheng-tang Liu ◽  
Li-ping Feng ◽  
Ning Li

2021 ◽  
Vol 11 (1) ◽  
Author(s):  
Maryam Zarghami Dehaghani ◽  
Fatemeh Molaei ◽  
Farrokh Yousefi ◽  
S. Mohammad Sajadi ◽  
Amin Esmaeili ◽  
...  

AbstractSimulation of thermal properties of graphene hetero-nanosheets is a key step in understanding their performance in nano-electronics where thermal loads and shocks are highly likely. Herein we combine graphene and boron-carbide nanosheets (BC3N) heterogeneous structures to obtain BC3N-graphene hetero-nanosheet (BC3GrHs) as a model semiconductor with tunable properties. Poor thermal properties of such heterostructures would curb their long-term practice. BC3GrHs may be imperfect with grain boundaries comprising non-hexagonal rings, heptagons, and pentagons as topological defects. Therefore, a realistic picture of the thermal properties of BC3GrHs necessitates consideration of grain boundaries of heptagon-pentagon defect pairs. Herein thermal properties of BC3GrHs with various defects were evaluated applying molecular dynamic (MD) simulation. First, temperature profiles along BC3GrHs interface with symmetric and asymmetric pentagon-heptagon pairs at 300 K, ΔT = 40 K, and zero strain were compared. Next, the effect of temperature, strain, and temperature gradient (ΔT) on Kaptiza resistance (interfacial thermal resistance at the grain boundary) was visualized. It was found that Kapitza resistance increases upon an increase of defect density in the grain boundary. Besides, among symmetric grain boundaries, 5–7–6–6 and 5–7–5–7 defect pairs showed the lowest (2 × 10–10 m2 K W−1) and highest (4.9 × 10–10 m2 K W−1) values of Kapitza resistance, respectively. Regarding parameters affecting Kapitza resistance, increased temperature and strain caused the rise and drop in Kaptiza thermal resistance, respectively. However, lengthier nanosheets had lower Kapitza thermal resistance. Moreover, changes in temperature gradient had a negligible effect on the Kapitza resistance.


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