Investigation on hydrogen dissociation pressure, heat of formation and strain energy of metal hydrides

2020 ◽  
Vol 840 ◽  
pp. 155686 ◽  
Author(s):  
Yoshitsugu Kojima ◽  
Masakuni Yamaguchi
1969 ◽  
Vol 91 (12) ◽  
pp. 3372-3373 ◽  
Author(s):  
Kenneth B. Wiberg ◽  
Elmer C. Lupton ◽  
George J. Burgmaier

1994 ◽  
Vol 116 (14) ◽  
pp. 6445-6446 ◽  
Author(s):  
Paul O. Staneke ◽  
Steen Ingemann ◽  
Philip Eaton ◽  
Nico M. M. Nibbering ◽  
Steven R. Kass

2012 ◽  
Vol 2012 ◽  
pp. 1-7 ◽  
Author(s):  
John A. Bumpus

The cage compound CL-20 (a.k.a., 2,4,6,8,10,12-hexanitro-2,4,6,8,10,12-hexaazaisowurtzitane, HNIW, or 2,4,6,8,10,12-hexanitro-2,4,6,8,10,12-hexaazatetracyclo[5.5.0.03,11.05,9]dodecane) is a well-studied high-energy-density material (HEDM). The high positive gas- (ΔfHg°) and solid- (ΔfHs°) phase heat of formation values for CL-20 conformers have often been attributed to the strain energy of this cage compound and, by implication, to the conventional ring strain energy (CRSE) inherent in isowurtzitane which may be viewed as a “parent compound” (although not the synthetic precursor) of CL-20. ΔfHg° values and destabilization energies (DSEs), which include the contribution from CRSE, were determined by computation using a relatively new multilevel ab intio model chemistry. Compared to cubane, isowurtzitane does not have an exceptionally high CRSE. It is about the same as that of cyclopropane and cyclobutane. These investigations demonstrate that instead of the CRSE inherent in the isowurtzitane parent compound, the relatively high ΔfHg° and DSE values of CL-20 conformers must be due, primarily, to torsional strain (Pitzer strain), transannular strain (Prelog strain), and van der Waals interactions that occur due to the presence of the six >N–NO2 substituents that replace the six methylene (–CH2–) groups in the isowurtzitane parent compound. These conclusions are even more pronounced when 2,4,6,8,10,12-hexaazaisowurtzitane is viewed as the “parent compound.”


1962 ◽  
Vol 84 (20) ◽  
pp. 3980-3981 ◽  
Author(s):  
Kenneth B. Wiberg ◽  
William J. Bartley ◽  
F. P. Lossing

2012 ◽  
Vol 554-556 ◽  
pp. 1618-1623 ◽  
Author(s):  
Xiu Lin Zeng ◽  
Xue Hai Ju ◽  
Hong Xu Gao

The heat of formation (HOF) for a caged owurtzitane analogue compound of 4,10-dinitro-2,6,8,12-tetraoxa-4,10-diaza-tetracyclododecane (TEX) was obtained by density functional theory B3LYP method with 6-31+G** basis set. The isodesmic reaction, instead of atomization reaction, makes good use of the available experimental data of HOFs and thus ensures the credibility of the result. The value of HOF of TEX is –448.37 kJ/mol. The predicted detonation velocity is about 8.2 km/s and detonation pressure is 31.44 GPa. The dissociation energy for the N-NO2 bond of TEX is 165.43 kJ/mol. There is large strain in TEX with strain energy of 62.47 kJ/mol. The nitro group interaction in TEX is small.


2005 ◽  
Vol 884 ◽  
Author(s):  
Yoshitsugu Kojima ◽  
Yasuaki Kawai ◽  
Shin-Ichi Towata ◽  
Tomoya Matsunaga ◽  
Tamio Shinozawa ◽  
...  

AbstractThe effective hydrogen capacity of TixCr2-yMny [≫X λ1.1 (1.08≤0x≤1.16), y λ1.0 (0.96≤y≤1.08)rsqb; exhibited the maximum value of 1.8 wt% in the pressure range of 33 MPa and 0.1 MPa at 296K (dissociation pressure: 5-11 MPa), and the alloy provided over 10% more capacity than conventional Ti-Cr-Mn (Ti1.2CrMn: 1.6 wt%, Ti1.2Cr1.9Mn0.1: 1.3 wt%). At the low temperature of 233 K, the alloy absorbed 2.0 wt% of hydrogen and the hydrogen desorption capacity at 0.1 MPa was 1.6 wt%. The dissociation pressure decreased with the Ti and the Mn contents and was explained by the function of the bulk modulus and the cell volume. According to the van't Hoff plots, the standard enthalpy differences (heat of formation) of the Ti1.16Cr0.92Mn1.08 and Ti1.08Cr1.04Mn0.96 hydrides were -21 and -22 kJ/molH2, respectively. These absolute values were about 10 kJ/molH2 smaller than those of LaNi5 and Ti-Cr-V. The alloy had sufficient hydriding and dehydriding kinetics. In the pressure range of 33 MPa and 0.1 MPa at 296 K, the alloy absorbed and desorbed 1.8 wt% of hydrogen in 60 sec and 300 sec, respectively. The hydrogen capacity changed gradually over many cycles and that after 1000 cycles was 94 % of the initial capacity. Thus Ti1.1CrMn can be utilized for a high- pressure MH tank which contains a hydrogen absorbing alloy with high dissociation pressure and compressed hydrogen.


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