Relation between Heat of Vaporization, Ion Transport, Molar Volume, and Cation−Anion Binding Energy for Ionic Liquids

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Oleg Borodin
Chemosphere ◽  
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Harrie A.J. Govers ◽  
Ronald Luijk ◽  
Erik H.G. Evers

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Matthew D. Green ◽  
Christian Schreiner ◽  
Timothy E. Long

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Ha Young Jung ◽  
Onnuri Kim ◽  
Moon Jeong Park

2016 ◽  
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Fei Fan ◽  
Weiyu Wang ◽  
Adam P. Holt ◽  
Hongbo Feng ◽  
David Uhrig ◽  
...  

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Danilo Rosa Nunes ◽  
Thomas G. Dane ◽  
Johan Jacquemin ◽  
Ulla Vainio ◽  
...  

2017 ◽  
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Venkat Ganesan

2019 ◽  
Vol 4 (2) ◽  
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Venkat Ganesan

Recent developments and outstanding questions in the context of charge transport mechanisms in polymeric ionic liquids are highlighted.


1989 ◽  
Vol 67 (1) ◽  
pp. 63-71 ◽  
Author(s):  
Magne Haugen ◽  
Erlend Østgaard

The ground-state energy of spin-polarized hydrogen, deuterium, and tritium is calculated by means of a modified variational lowest order constrained-variation method, and the calculations are done for five different two-body potentials. Spin-polarized H↓ is not self-bound according to our theoretical results for the ground-state binding energy. For spin-polarized D↓, however, we obtain theoretical results for the ground-state binding energy per particle from −0.42 K at an equilibrium particle density of 0.25 σ−3 or a molar volume of 121 cm3/mol to + 0.32 K at an equilibrium particle density of 0.21 σ−3 or a molar volume of 142 cm3/mol, where σ = 3.69 Å (1 Å = 10−10 m). It is, therefore, not clear whether spin-polarized deuterium should be self-bound or not. For spin-polarized T↓, we obtain theoretical results for the ground-state binding energy per particle from −4.73 K at an equilibrium particle density of 0.41 σ−3 or a molar volume of 74 cm3/mol to −1.21 K at an equilibrium particle density of 0.28 σ−3 or a molar volume of 109 cm3/mol.


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