<p>The solid-phase enthalpy of formation (∆H<sub><i>f</i>, <i>solid</i></sub>) of energetic materials was generally predicted from the gas-phase enthalpy of formation (∆H<sub><i>f, gas</i></sub>) and sublimation enthalpy (∆H<sub><i>sub</i></sub>). Here, the standard ∆H<sub><i>f, solid</i></sub> of energetic materials is directly obtained from density functional theory (DFT) calculations by computing the enthalpy difference between the solid-phase energetic material and its constituent elements in their reference states. To reduce the errors in DFT calculations, a concept of isocoordinated reaction is introduced, i.e., the reference states are selected based on the coordination numbers of all atoms in the energetic material. This DFT method for ∆H<sub><i>f, solid</i></sub> calculation does not require experimental input, data fitting, or machine learning. For more than 150 energetic materials collected from the literature, the mean absolute error (MAE) of ∆H<sub><i>f, solid</i></sub> for the DFT method is 39 kJ mol<sup>−1</sup> (or 9.3 kcal mol<sup>−1</sup>) referring to the literature. Our demonstration raises prospects for first-principles prediction of the properties of energetic materials, and the proposed method for ∆H<sub><i>f, solid</i></sub> calculation is also promising for other materials.</p>

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First-principles calculations of solid-phase enthalpy of formation of energetic materials

  • Lixiang Zhong,
  • Danyang Liu,
  • Maoxin Hu,
  • Xiaoning Yang,
  • Ruibin Liu,
  • Yugui Yao

摘要

The solid-phase enthalpy of formation (∆Hf, solid) of energetic materials was generally predicted from the gas-phase enthalpy of formation (∆Hf, gas) and sublimation enthalpy (∆Hsub). Here, the standard ∆Hf, solid of energetic materials is directly obtained from density functional theory (DFT) calculations by computing the enthalpy difference between the solid-phase energetic material and its constituent elements in their reference states. To reduce the errors in DFT calculations, a concept of isocoordinated reaction is introduced, i.e., the reference states are selected based on the coordination numbers of all atoms in the energetic material. This DFT method for ∆Hf, solid calculation does not require experimental input, data fitting, or machine learning. For more than 150 energetic materials collected from the literature, the mean absolute error (MAE) of ∆Hf, solid for the DFT method is 39 kJ mol−1 (or 9.3 kcal mol−1) referring to the literature. Our demonstration raises prospects for first-principles prediction of the properties of energetic materials, and the proposed method for ∆Hf, solid calculation is also promising for other materials.