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Heat Capacities of an Ideal Gas III01:25

Heat Capacities of an Ideal Gas III

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The number of independent ways a gas molecule can move along straight line, rotate, and vibrate is called its degrees of freedom. Supposing d represents the number of degrees of freedom of an ideal gas, the molar heat capacity at constant volume of an ideal gas in terms of d is
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Heat Capacities of an Ideal Gas II01:23

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For a system that undergoes a thermodynamic process at a constant volume condition, the heat absorbed is used only to increase the system's internal energy and not for doing any kind of work. While for a system undergoing a thermodynamic process under a constant pressure condition, the amount of heat absorbed is used not only for increasing the internal energy (as a function of temperature) but also for doing some work. The molar heat capacity is the amount of heat required to increase the...
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Heat Capacities of an Ideal Gas I01:14

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Heat capacity is the ratio of heat absorbed by the substance corresponding to its temperature change. It is also called thermal capacity and the SI unit of heat capacity is J/K. Whereas, specific heat capacity is defined as the amount of heat necessary to change the temperature of 1 kg of a substance by 1 K and is also called massic heat capacity. Its SI unit is J/kg⋅K.
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Maxwell-Boltzmann Distribution: Problem Solving01:20

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Individual molecules in a gas move in random directions, but a gas containing numerous molecules has a predictable distribution of molecular speeds, which is known as the Maxwell-Boltzmann distribution, f(v).
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Atomic Nuclei: Nuclear Spin State Population Distribution01:14

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Near absolute zero temperatures, in the presence of a magnetic field, the majority of nuclei prefer the lower energy spin-up state to the higher energy spin-down state. As temperatures increase, the energy from thermal collisions distributes the spins more equally between the two states. The Boltzmann distribution equation gives the ratio of the number of spins predicted in the spin −½ (N−) and spin +½ (N+) states.
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Kinetic Theory of an Ideal Gas01:12

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A mole is defined as the amount of any substance that contains as many molecules as there are atoms in exactly 12 grams of carbon-12. An Italian scientist Amedeo Avogadro (1776–1856) formed the  hypothesis that equal volumes of gas at equal pressure and temperature contain equal numbers of molecules, independent of the type of gas. Later, the hypothesis was developed to form the SI unit for measuring the amount of any substance.
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Non-equilibrium Microwave Plasma for Efficient High Temperature Chemistry
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Real-space density kernel method for Kohn-Sham density functional theory calculations at high temperature.

Qimen Xu1, Xin Jing1, Boqin Zhang1

  • 1College of Engineering, Georgia Institute of Technology, Atlanta, Georgia 30332, USA.

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|March 9, 2022
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High-temperature Kohn-Sham calculations are accelerated by a new density matrix method, eliminating costly diagonalization. This approach significantly reduces computational expense for electronic structure studies.

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Area of Science:

  • Computational Physics
  • Materials Science
  • Quantum Chemistry

Background:

  • Kohn-Sham density functional theory (KS-DFT) calculations become computationally intensive at high temperatures.
  • Conventional diagonalization methods require computing numerous partially occupied states, increasing costs.
  • Efficient methods are needed for high-temperature electronic structure simulations.

Purpose of the Study:

  • To develop a computationally efficient density matrix-based method for high-temperature KS-DFT.
  • To eliminate the need for expensive diagonalization steps in KS-DFT calculations.
  • To enable accurate simulations of materials at extreme temperatures.

Main Methods:

  • A density matrix-based approach for Kohn-Sham calculations at high temperatures.
  • Development of real-space expressions for electron density, free energy, forces, and stress tensor.
  • Utilizing Chebyshev filtering to generate an auxiliary orbital basis.
  • Employing spectral quadrature techniques for density kernel, band structure, and entropic energy calculations.
  • Implementation within the SPARC electronic structure code.

Main Results:

  • The new method significantly reduces computational cost by avoiding diagonalization.
  • Systematic convergence of calculated quantities to exact diagonalization results was demonstrated.
  • Significant speedups were achieved compared to conventional diagonalization methods.
  • Accurate computation of aluminum's self-diffusion coefficient and viscosity at 116,045 K.

Conclusions:

  • The presented density matrix method offers a substantial speedup for high-temperature KS-DFT.
  • The method provides accurate results, comparable to traditional diagonalization techniques.
  • This approach facilitates advanced quantum molecular dynamics simulations at extreme conditions.