EPSRC's High End Computing Programme. We acknowledge the support of the Diamond Light Source, STFC, and the ISIS Neutron and Muon Facility.
Supporting information:The remaining DSC thermograms for β-RDX (Figures S1−S4); a comparison between the calculated lattice parameters and unit cell volumes for α-and γ-RDX, compared to previous DFT-D studies as well as relevant experimental data ( Figures S5 and S6); comparison of predicted INS spectra for α-RDX to those for γ-and ε-RDX at similar pressures ( Figures S7 and S8); a comparison of the DFT-D predicted crystallographic parameters with corresponding experimental data for α-, γ-, and ε-RDX (Tables S1, S3, and S4, respectively); full lists of calculated phonon modes as a function of pressure for α-, γ-, and ε-RDX compared to experimental Raman data, including pressure-induced shift values (Tables S2, S5, and S6). This material is available free of charge via the Internet at http://pubs.acs.org
Graphical abstract:
Abstract:We have performed simulations utilizing the dispersion-corrected density functional theory method (DFT-D) as parametrized by Grimme on selected polymorphs of RDX (cyclotrimethylenetrinitramine). Additionally, we present the first experimental determination of the enthalpy of fusion (ΔH fus ) of the highly metastable β-form of RDX. The characteristics of fusion for β-RDX were determined to be 186.7 ± 0.8 °C, 188.5 ± 0.4 °C, and 12.63 ± 0.28 kJ mol -1 for the onset temperature, peak temperature (or melting point), and ΔH fus , respectively. The difference in experimental ΔH fus for the α-and β-forms of RDX is 20.46 ± 0.92 kJ mol -1 . Ambient-pressure lattice energies (E L ) of the α-and β-forms of RDX have been calculated and are in excellent agreement with experiment. In addition the computationally predicted difference in E L (20.35 kJ mol -1 ) between the α-and β-forms is in excellent agreement with the experimental difference in ΔH fus . The response of the lattice parameters and unit-cell volumes to pressure for the α-and γ-forms have been investigated, in addition to the first high-pressure computational study of the ε-form of RDX-these results are in very good agreement with experimental data. Phonon calculations provide good agreement for vibrational frequencies obtained from Raman spectroscopy, and a predicted inelastic neutron scattering (INS) spectrum of α-RDX shows excellent agreement with experimental INS data determined in this study. The transition energies and intensities are reproduced, confirming that both the eigenvalues and the eigenvectors of the vibrations are correctly described by the DFT-D method. The results of the high-pressure phonon calculations have been used to show that the heat capacities of the α-, γ-, and ε-forms of RDX are only weakly affected by pressure.
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