Organic Molecular Crystals: From Non-Porous Structure to Potential Porous Structure Controlled by Reaction Temperature

2014 ◽  
Vol 67 (11) ◽  
pp. 1675
Author(s):  
Xiao-Liu Wu ◽  
Ming-Biao Luo ◽  
Jian-Qiang Li ◽  
Yan Zhu ◽  
Feng Luo

Reported here are two novel organic crystals, L 1 and L·(DMF)1.5 2 (DMF = (CH3)2NCHO), showing non-porous and microporous structure, where the formations can be precisely controlled by varying the reaction temperature. The reason for this exciting discovery could be directly related to the various degrees of distortion in the organic molecules as observed in 1 and 2, where detailed structural studies were carried out.

2016 ◽  
Vol 18 (23) ◽  
pp. 15828-15837 ◽  
Author(s):  
Jonas Nyman ◽  
Orla Sheehan Pundyke ◽  
Graeme M. Day

We assess a series of atom–atom force fields for lattice energy and free energy modelling of molecular organic crystals.


RSC Advances ◽  
2015 ◽  
Vol 5 (79) ◽  
pp. 64156-64162 ◽  
Author(s):  
Reda M. Mohamed ◽  
Manish Kumar Mishra ◽  
Laila M. AL-Harbi ◽  
Mohammed S. Al-Ghamdi ◽  
Upadrasta Ramamurty

Nanoindentation technique was employed on organic molecular crystals to investigate how the anisotropy in the mechanical behavior changes within the temperature range of 283 to 343 K.


2016 ◽  
Vol 18 (44) ◽  
pp. 30313-30322 ◽  
Author(s):  
Ian J. Nessler ◽  
Jacob M. Litman ◽  
Michael J. Schnieders

First principles prediction of the structure, thermodynamics and solubility of organic molecular crystals, which play a central role in chemical, material, pharmaceutical and engineering sciences, challenges both potential energy functions and sampling methodologies.


1995 ◽  
Vol 60 (2) ◽  
pp. 172-187 ◽  
Author(s):  
Pavel Fott ◽  
František Kolář ◽  
Zuzana Weishauptová

On carbonizing phenolic resins, the development of porous structure takes place which influences the transport properties of carbonized materials. To give a true picture of this effect, specimens in the shape of plates were prepared and carbonized at various temperatures. The carbonizates obtained were studied by adsorption methods, electron microscopy, and mercury porosimetry. Diffusivities were evaluated in terms of measuring the kinetics of wetting and drying. It was found out that the porous structure of specimens in different stages of carbonization is formed mostly by micropores whose volumes were within 0.06 to 0.22 cm3/g. The maximum micropore volume is reached at the temperature of 750 °C. The dependence of diffusivity on the carbonization temperature is nearly constant at first, begins to increase in the vicinity of 400 °C, and at 600 °C attains its maximum. The experimental results reached are in agreement with the conception of the development and gradual closing of the microporous structure in the course of carbonization. The dependence of diffusivity on temperature can be expressed by the Arrhenius equation. In this connection, two possible models of mass transport were discussed.


1995 ◽  
Vol 94 (12) ◽  
pp. 1013-1018 ◽  
Author(s):  
Itaru Tsukushi ◽  
Osamu Yamamuro ◽  
Takasuke Matsuo

2021 ◽  
Vol 125 (4) ◽  
pp. 1012-1024
Author(s):  
Miguel Rivera ◽  
Ljiljana Stojanović ◽  
Rachel Crespo-Otero

Materials ◽  
2021 ◽  
Vol 14 (11) ◽  
pp. 2951
Author(s):  
Mirosław Kwiatkowski ◽  
Jarosław Serafin ◽  
Andy M. Booth ◽  
Beata Michalkiewicz

This paper presents the results of a computer analysis of the effect of activation process temperature on the development of the microporous structure of activated carbon derived from the leaves of common polypody (Polypodium vulgare) via chemical activation with phosphoric acid (H3PO4) at activation temperatures of 700, 800, and 900 °C. An unconventional approach to porous structure analysis, using the new numerical clustering-based adsorption analysis (LBET) method together with the implemented unique gas state equation, was used in this study. The LBET method is based on unique mathematical models that take into account, in addition to surface heterogeneity, the possibility of molecule clusters branching and the geometric and energy limitations of adsorbate cluster formation. It enabled us to determine a set of parameters comprehensively and reliably describing the porous structure of carbon material on the basis of the determined adsorption isotherm. Porous structure analyses using the LBET method were based on nitrogen (N2), carbon dioxide (CO2), and methane (CH4) adsorption isotherms determined for individual activated carbon. The analyses carried out showed the highest CO2 adsorption capacity for activated carbon obtained was at an activation temperature of 900 °C, a value only slightly higher than that obtained for activated carbon prepared at 700 °C, but the values of geometrical parameters determined for these activated carbons showed significant differences. The results of the analyses obtained with the LBET method were also compared with the results of iodine number analysis and the results obtained with the Brunauer–Emmett–Teller (BET), Dubinin–Radushkevich (DR), and quenched solid density functional theory (QSDFT) methods, demonstrating their complementarity.


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