The electronic and vibrational structures of C,, and C,,, have been calculated at the PM3 semiempirical level. C, has a partially delocalized structure, while C,, has both a localized set and a delocalized set of MOs. As with AM1 and MNDO, PM3 predicts the heat of formation of C,, to be greater than that of C,,,, and that C,,, is the thermodynamically more stable species. Calculation of the normal modes was accelerated over 40 times by limited use of symmetry theory.
The deuterium isotope effect was applied to condensed-phase thermochemical reactions of HMX and HMX-8 by using isothermal techniques. Dissimilar deuterium isotope effects revealed a mechanistic dependence of HMX upon different physical states which may singularly predominate in a specific type of thermal event. Solid-state HMX thermochemical decomposition produces a primary deuterium isotope effect (DIE), indicating that covalent C-H bond rupture is the rate-controlling step in this phase. An apparent inverse DIE is displayed by the mixed melt phase and can be attributed to C-H bond contraction during a weakening of molecular lattice forces as the solid HMX liquefies. The liquid-state decomposition rate appears to be controlled by ring C-N bond cleavage as evidenced by a secondary DIE and higher molecular weight products. These results reveal a dependence of the HMX decomposition process on physical state and lead to a broader mechanistic interpretation which explains the seemingly contradictory data found in current literature reviews.
MIND0/3, MNDO, AM1, and PM3 calculations of molecular vibrational frequencies are reported for 61 molecules. All techniques were applied to both well-behaved and badly behaved systems. Overall, MIND0/3 and MNDO were found to contain rather large errors whereas AM1 and PM3 were relatively accurate. Since no technique does well for all molecules, the technique used should be chosen based on the molecular vibration of interest. in general, AM1 and PM3 together provide fairly accurate resuits.
The structures and thermodynamic stabilities of X(YH4)3, X and/or Y being boron or aluminum, were calculated using ab initio molecular orbital methods. The structures were determined at the Hartree-Fock level using the 6-31G* basis set and confirmed to be minima by vibrational analysis. Correlation effects were estimated using MP4(SDTQ) calculations at the Hartree-Fock minima. The correlated energies were used to estimate AH0 and AG°for the decomposition of these dodecahydrides into various products. No Hartree-Fock minimum could be found for B(A1H4)3. The symmetries of the other structures were found to be rotated prisms. Only A1(BH4)3, which is known experimentally, was stable with respect to all the decomposition modes studied. Comparison of the calculated vibrational spectra of these dodecahydrides with those of analogous covalently bonded molecules and ionically bonded molecules suggests that B(BH4)3, A1(BH4)3, and A1(A1H4)3 are all primarily covalently bonded.
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