Determination of Thermal Conductivity of Inorganic Salts at the Liquid/Solid Phase Transition Point

Author(s):  
Zhan Shuiqing ◽  
Wu Ye ◽  
Zhou Jiemin ◽  
Yang Ying ◽  
Liang Yannan ◽  
...  
2019 ◽  
Vol 21 (24) ◽  
pp. 13070-13077 ◽  
Author(s):  
Jianxiang Tian ◽  
Hua Jiang ◽  
A. Mulero

A review on the numerical virial coefficients, compressibility factor, fluid–solid phase transition point and equations of the state of hard sphere fluids.


1998 ◽  
Vol 13 (18) ◽  
pp. 3193-3202
Author(s):  
XITE ZHENG

A variational calculation scheme of SU (N) lattice gauge Wilson models for large but finite N is presented. The order parameter EP and the phase transition points of lattice SU (N) gauge systems for N=4~6 are calculated. The results are in good agreement with Monte Carlo simulations. An extrapolation procedure for determination of the phase transition point in the large N limit is proposed.


MRS Advances ◽  
2018 ◽  
Vol 3 (54) ◽  
pp. 3213-3220
Author(s):  
Yulong Wu ◽  
Peng Meng ◽  
Quan Zhang ◽  
Zhiyuan Tan ◽  
Guoan Cheng ◽  
...  

ABSTRACTThe room-temperature switching effect is of great interest for many applications, such as smart buildings, sensors, thermal energy storage and automatic temperature control. In this paper, we report a room-temperature switchable carbon nanotube (CNT)/hexadecane composites. Electrical conductivity, thermal conductivity and permittivity of the CNT/hexadecane composites can be regulated around 18°C and the maximal switching ratio reaches 5 orders of magnitude, 3 times and 106.4, respectively. The switching behavior of composites is caused by rearrangement of the carbon nanotube fillers in hexadecane matrix during liquid-solid phase transition. It is found that surface modification is necessary to improve dispersion stability. Effects of filler properties on switching behaviour are also discussed.


RSC Advances ◽  
2017 ◽  
Vol 7 (54) ◽  
pp. 33775-33781 ◽  
Author(s):  
Keshab Dahal ◽  
Qian Zhang ◽  
Yumei Wang ◽  
Ishwar Kumar Mishra ◽  
Zhifeng Ren

An increase in thermal conductivity is achieved by increasing electronic thermal conductivityviamodulation doping, resulting from solid–solid phase transition.


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