Matches in SemOpenAlex for { <https://semopenalex.org/work/W1999463389> ?p ?o ?g. }
- W1999463389 abstract "The phonon spectra of $ensuremath{alpha}$, $ensuremath{beta}$, and $ensuremath{omega}$ Ti were studied using the supercell approach. The lattice vibrational energy was calculated in the quasiharmonic approximation using both first-principles phonon density of state and Debye model. The thermal electronic contribution to the free energy was evaluated from the integration over the electronic density of states. The Helmholtz energy was thus obtained by combining them with the 0 K total energy calculated within the framework of all-electron projector-augmented-wave method. The thermodynamic properties of $ensuremath{alpha}$ and $ensuremath{omega}$ Ti calculated by phonon and Debye model are very close to each other. The predicted enthalpy, entropy, bulk modulus, thermal expansion coefficient and heat capacity of $ensuremath{alpha}$ are in good agreement with experiments. By comparing with the experimental enthalpy of $ensuremath{beta}$, we found that the 0 K total energy calculated from bcc Ti is incorrect. This problem can be solved by shifting the total energy of $ensuremath{beta}$ down by $8text{ }text{kJ}text{ }{text{mol}}^{ensuremath{-}1}$ to match the experimental value. With the Gibbs energy calculated from the Debye model as a function of pressure and temperature, the phase transformation conditions of $ensuremath{alpha}ensuremath{rightarrow}ensuremath{omega}$, $ensuremath{alpha}ensuremath{rightarrow}ensuremath{beta}$, and $ensuremath{beta}ensuremath{rightarrow}ensuremath{omega}$ were identified. The predicted transition temperature between $ensuremath{alpha}$ and $ensuremath{beta}$ at ambient pressure and the triple point are close to experiments. It was found that the entropy plays an important role in the $ensuremath{omega}ensuremath{rightarrow}ensuremath{alpha}$ and $ensuremath{alpha}ensuremath{rightarrow}ensuremath{beta}$ transitions, and the thermal electronic contribution to the Gibbs energy cannot be neglected for studying the $ensuremath{alpha}ensuremath{rightarrow}ensuremath{beta}$ transition. Our calculations also showed that zero-point energy is crucial to predict the transition pressure of Ti at low temperatures." @default.
- W1999463389 created "2016-06-24" @default.
- W1999463389 creator A5059583846 @default.
- W1999463389 creator A5076627740 @default.
- W1999463389 creator A5087326200 @default.
- W1999463389 creator A5091161457 @default.
- W1999463389 date "2009-09-24" @default.
- W1999463389 modified "2023-10-01" @default.
- W1999463389 title "Density-functional study of the thermodynamic properties and the pressure–temperature phase diagram of Ti" @default.
- W1999463389 cites W116239404 @default.
- W1999463389 cites W1546841433 @default.
- W1999463389 cites W1573968521 @default.
- W1999463389 cites W1965459801 @default.
- W1999463389 cites W1967539050 @default.
- W1999463389 cites W1970017339 @default.
- W1999463389 cites W1970127494 @default.
- W1999463389 cites W1975437393 @default.
- W1999463389 cites W1979544533 @default.
- W1999463389 cites W1981368803 @default.
- W1999463389 cites W1982133696 @default.
- W1999463389 cites W1983008001 @default.
- W1999463389 cites W1987207774 @default.
- W1999463389 cites W1988762313 @default.
- W1999463389 cites W1998927827 @default.
- W1999463389 cites W2008319486 @default.
- W1999463389 cites W2013557865 @default.
- W1999463389 cites W2018924230 @default.
- W1999463389 cites W2022478067 @default.
- W1999463389 cites W2034227993 @default.
- W1999463389 cites W2041308859 @default.
- W1999463389 cites W2041914615 @default.
- W1999463389 cites W2053426080 @default.
- W1999463389 cites W2058523970 @default.
- W1999463389 cites W2062563005 @default.
- W1999463389 cites W2063394478 @default.
- W1999463389 cites W2065451819 @default.
- W1999463389 cites W2067398151 @default.
- W1999463389 cites W2070686939 @default.
- W1999463389 cites W2074189430 @default.
- W1999463389 cites W2077150921 @default.
- W1999463389 cites W2083222334 @default.
- W1999463389 cites W2087126020 @default.
- W1999463389 cites W2105384912 @default.
- W1999463389 cites W2110329024 @default.
- W1999463389 cites W2150662901 @default.
- W1999463389 cites W2317161978 @default.
- W1999463389 cites W2989006667 @default.
- W1999463389 cites W4249855967 @default.
- W1999463389 cites W4253121421 @default.
- W1999463389 cites W7030554 @default.
- W1999463389 doi "https://doi.org/10.1103/physrevb.80.104116" @default.
- W1999463389 hasPublicationYear "2009" @default.
- W1999463389 type Work @default.
- W1999463389 sameAs 1999463389 @default.
- W1999463389 citedByCount "91" @default.
- W1999463389 countsByYear W19994633892012 @default.
- W1999463389 countsByYear W19994633892013 @default.
- W1999463389 countsByYear W19994633892014 @default.
- W1999463389 countsByYear W19994633892015 @default.
- W1999463389 countsByYear W19994633892016 @default.
- W1999463389 countsByYear W19994633892017 @default.
- W1999463389 countsByYear W19994633892018 @default.
- W1999463389 countsByYear W19994633892019 @default.
- W1999463389 countsByYear W19994633892020 @default.
- W1999463389 countsByYear W19994633892021 @default.
- W1999463389 countsByYear W19994633892022 @default.
- W1999463389 countsByYear W19994633892023 @default.
- W1999463389 crossrefType "journal-article" @default.
- W1999463389 hasAuthorship W1999463389A5059583846 @default.
- W1999463389 hasAuthorship W1999463389A5076627740 @default.
- W1999463389 hasAuthorship W1999463389A5087326200 @default.
- W1999463389 hasAuthorship W1999463389A5091161457 @default.
- W1999463389 hasConcept C121332964 @default.
- W1999463389 hasConcept C146477669 @default.
- W1999463389 hasConcept C24169881 @default.
- W1999463389 hasConcept C25376523 @default.
- W1999463389 hasConcept C26873012 @default.
- W1999463389 hasConcept C27592594 @default.
- W1999463389 hasConcept C2779557605 @default.
- W1999463389 hasConcept C3288061 @default.
- W1999463389 hasConcept C44280652 @default.
- W1999463389 hasConcept C60205243 @default.
- W1999463389 hasConcept C62520636 @default.
- W1999463389 hasConcept C85906118 @default.
- W1999463389 hasConcept C94406020 @default.
- W1999463389 hasConcept C97355855 @default.
- W1999463389 hasConceptScore W1999463389C121332964 @default.
- W1999463389 hasConceptScore W1999463389C146477669 @default.
- W1999463389 hasConceptScore W1999463389C24169881 @default.
- W1999463389 hasConceptScore W1999463389C25376523 @default.
- W1999463389 hasConceptScore W1999463389C26873012 @default.
- W1999463389 hasConceptScore W1999463389C27592594 @default.
- W1999463389 hasConceptScore W1999463389C2779557605 @default.
- W1999463389 hasConceptScore W1999463389C3288061 @default.
- W1999463389 hasConceptScore W1999463389C44280652 @default.
- W1999463389 hasConceptScore W1999463389C60205243 @default.
- W1999463389 hasConceptScore W1999463389C62520636 @default.
- W1999463389 hasConceptScore W1999463389C85906118 @default.
- W1999463389 hasConceptScore W1999463389C94406020 @default.
- W1999463389 hasConceptScore W1999463389C97355855 @default.