Search NASA⌕ Search

DOE OSTI · 2585296

First principles free energy model with dynamic magnetism for δ -plutonium

Abstract

We present an ab initio free energy model derived from a fully relativistic density functional theory (DFT) electronic structure with dynamic magnetism for δ -plutonium (face-centered cubic, fcc). The DFT model is extended with orbital-orbital interaction in a parameter free orbital polarization (OP) mechanism consistent with previous modeling of plutonium. Gibbs free energy is built from components associated with the temperature dependence of the electronic structure and the corresponding electronic entropy, lattice vibrations within an anharmonic lattice dynamics model, and dynamical fluctuations of the magnetization density, i.e. magnetic fluctuations. The fluctuation model consists of transverse and longitudinal modes driven by temperature induced excitations of the DFT + OP electronic structure. The ab initio model thus incorporates fluctuating states beyond the electronic ground state. Thanks to the dynamic magnetism, the theory predicts excellent thermodynamic properties and a Gibbs free energy in accord with CALPHAD and semi-empirical modeling developed from the thermodynamic observables. The magnetic fluctuations further explain anomalous behaviors of the thermal expansion in plutonium. Specifically, a thermal expansion for the δ -plutonium system turning from positive to negative at temperatures above room temperature, a tendency for gallium to reduce and remove the negative thermal expansion depending on composition, and a positive thermal expansion for the high temperature ϵ phase.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

Söderlind, Per [Lawrence Livermore National Laboratory (LLNL), Livermore, CA (United States)] (ORCID:0000000236386617), Landa, Alexander [Lawrence Livermore National Laboratory (LLNL), Livermore, CA (United States)] (ORCID:0000000292169422), Benedict, Lorin X. [Lawrence Livermore National Laboratory (LLNL), Livermore, CA (United States)] (ORCID:0000000275650230), Goldman, Nir [Lawrence Livermore National Laboratory (LLNL), Livermore, CA (United States)] (ORCID:0000000330522128), Hood, Randolph Q. [Lawrence Livermore National Laboratory (LLNL), Livermore, CA (United States)] (ORCID:000000031806104X), Kweon, Kyoung Eun [Lawrence Livermore National Laboratory (LLNL), Livermore, CA (United States)] (ORCID:0000000151553789), Moore, Emily E. [Lawrence Livermore National Laboratory (LLNL), Livermore, CA (United States)] (ORCID:0000000266982292), Perron, Aurelien [Lawrence Livermore National Laboratory (LLNL), Livermore, CA (United States)] (ORCID:000000025280003X), Sadigh, Babak [Lawrence Livermore National Laboratory (LLNL), Livermore, CA (United States)] (ORCID:0000000284877859), Wu, Christine J. [Lawrence Livermore National Laboratory (LLNL), Livermore, CA (United States)] (ORCID:0000000227686415), Yang, Lin H. [Lawrence Livermore National Laboratory (LLNL), Livermore, CA (United States)] (ORCID:0000000209546240). 2025-07-21. First principles free energy model with dynamic magnetism for δ -plutonium. https://doi.org/10.1088/1361-6633%2Fadedb1

Cite the original work for its findings. Save a collection to share your selection of sources.

KEEP EXPLORING

Related reports

Optimization of an Impedance-Matched Test Fixture with the Modal Projection Error

Across many industries and engineering disciplines, components and systems are designed and deployed into their operational environment of intended use. It is the desire of the design agency to be able to predict whether their component or system will function in its shock and vibration environments or if it will fail due to mechanical stresses. One method to determine if the component will survive the shock and vibration environments is to expose the component to the operational environment in a laboratory. One difficulty in executing a representative laboratory test is that the component may not have the same boundary condition in the laboratory as in the operational configuration. This paper examines the use of parameterized optimization to design the test fixture in order to better match the operational configuration. Several frequency and modal-based objective functions are examined for the optimization. The study shows that the Modal Projection Error objective function performs the best of the functions studied. The efficacy of the Modal Projection Error is demonstrated with respect to dynamic test fixture design on several analytical and experimental exemplars.

dynamic↗