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Thermodynamic Potentials01:26

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Thermodynamic potentials are state functions that are extremely useful in analyzing a thermodynamic system. They have dimensions of energy. The four important thermodynamic potentials are internal energy, enthalpy, Helmholtz free energy, and Gibbs free energy. These thermodynamic potentials can be expressed using two of the following variables: pressure, volume, temperature, and entropy. These two variables are expressed as the rate of change of the thermodynamic potential with respect to other...
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The free energy change for a reaction that occurs under the standard conditions of 1 bar pressure and at 298 K is called the standard free energy change. Since free energy is a state function, its value depends only on the conditions of the initial and final states of the system. A convenient and common approach to the calculation of free energy changes for physical and chemical reactions is by use of widely available compilations of standard state thermodynamic data. One method involves the...
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The ideal gas law is an approximation that works well at high temperatures and low pressures. The van der Waals equation of state (named after the Dutch physicist Johannes van der Waals, 1837−1923) improves it by considering two factors.
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The free energy change for a process taking place with reactants and products present under nonstandard conditions (pressures other than 1 bar; concentrations other than 1 M) is related to the standard free energy change according to this equation:
 
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Atoms and molecules interact with each other through intermolecular forces. These electrostatic forces arise from attractive or repulsive interactions between particles with permanent, partial, or temporary charges. The intermolecular forces between neutral atoms and molecules are ion–dipole, dipole–dipole, and dispersion forces, collectively known as van der Waals forces.
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Framework for Laplacian-Level Noninteracting Free-Energy Density Functionals.

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A new orbital-free meta-generalized-gradient approximation (meta-GGA) framework improves accuracy for thermal density functional theory simulations. This advanced method is particularly effective for warm dense matter at lower temperatures.

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Area of Science:

  • Computational Physics
  • Quantum Chemistry
  • Materials Science

Background:

  • Orbital-free density functional theory (DFT) methods offer computational efficiency but often lack accuracy, especially for thermal properties.
  • Existing approximations, like Thomas-Fermi and generalized gradient approximations (GGA), have limitations in describing complex systems.
  • Developing accurate orbital-free functionals is crucial for simulating systems under extreme conditions, such as warm dense matter.

Purpose of the Study:

  • To develop a novel framework for orbital-free meta-generalized-gradient approximation (meta-GGA) functionals.
  • To construct a nonempirical meta-GGA functional applicable to noninteracting free-energy-density functionals.
  • To enhance the accuracy of orbital-free DFT simulations for thermal properties.

Main Methods:

  • Development of a theoretical framework based on the fourth-order gradient expansion of the noninteracting free energy.
  • Construction of a nonempirical meta-GGA functional that reduces to known limits.
  • Application and validation of the new functional using simulations of warm dense helium.

Main Results:

  • A new orbital-free meta-GGA framework and a corresponding nonempirical functional were successfully developed.
  • The developed functional accurately reproduces the fourth-order gradient expansion in the slowly varying density limit.
  • Simulations of warm dense helium showed a drastic increase in accuracy below 40 eV compared to Thomas-Fermi and GGA methods.

Conclusions:

  • The developed orbital-free meta-GGA framework provides a significant advancement for thermal DFT calculations.
  • This new functional offers a more accurate description of warm dense matter at lower temperatures.
  • The study presents a valuable tool for future research in computational physics and materials science.