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Related Concept Videos

Scaling01:26

Scaling

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In designing and analyzing filters, resonant circuits, or circuit analysis at large, working with standard element values like 1 ohm, 1 henry, or 1 farad can be convenient before scaling these values to more realistic figures. This approach is widely utilized by not employing realistic element values in numerous examples and problems; it simplifies mastering circuit analysis through convenient component values. The complexity of calculations is thereby reduced, with the understanding that...
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The Van der Waals Equation01:26

The Van der Waals Equation

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The ideal gas law is based on two simplifying assumptions: first, that there are no intermolecular attractions between gas molecules, and second, that the volume occupied by the molecules themselves is negligible compared with the volume of the container. However, these assumptions don't hold up under all conditions - specifically, at high pressures and low temperatures, as gas tends to deviate from ideal gas behavior.The van der Waals equation is an enhanced version of the ideal gas law,...
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Van der Waals Equation01:10

Van der Waals Equation

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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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Real Gases: Effects of Intermolecular Forces and Molecular Volume Deriving Van der Waals Equation04:01

Real Gases: Effects of Intermolecular Forces and Molecular Volume Deriving Van der Waals Equation

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Thus far, the ideal gas law, PV = nRT, has been applied to a variety of different types of problems, ranging from reaction stoichiometry and empirical and molecular formula problems to determining the density and molar mass of a gas. However, the behavior of a gas is often non-ideal, meaning that the observed relationships between its pressure, volume, and temperature are not accurately described by the gas laws.
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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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Kinetic Theory of an Ideal Gas01:12

Kinetic Theory of an Ideal Gas

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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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Efficient Linear-Scaling Density Functional Theory for Molecular Systems.

Rustam Z Khaliullin1,2, Joost VandeVondele3, Jürg Hutter1

  • 1Physical Chemistry Institute, University of Zürich , Winterthurerstrasse 180, 8057 Zürich, Switzerland.

Journal of Chemical Theory and Computation
|November 22, 2015
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Summary
This summary is machine-generated.

New linear scaling (LS) density functional theory (DFT) methods use nonorthogonal localized orbitals to reduce computational cost. These efficient LS-DFT approaches enable accurate simulations of significantly larger molecular systems.

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Area of Science:

  • Computational Chemistry
  • Quantum Chemistry
  • Materials Science

Background:

  • Density Functional Theory (DFT) is a powerful quantum mechanical modeling method.
  • Linear scaling (LS) DFT methods aim to reduce the computational cost of traditional DFT.
  • Existing LS-DFT methods still face high computational overhead, limiting their widespread application.

Purpose of the Study:

  • To develop novel, computationally efficient linear scaling (LS) density functional theory (DFT) methods.
  • To overcome the high computational cost associated with current LS-DFT techniques.
  • To enable accurate DFT simulations for larger molecular systems than previously feasible.

Main Methods:

  • Exploitation of nonorthogonal localized molecular orbitals.
  • Development of a robust two-stage variational procedure for optimization.
  • Implementation of an accurate nonself-consistent approach as an alternative to optimization.

Main Results:

  • The proposed LS-DFT methods exhibit significantly lower computational overhead.
  • High efficiency was achieved through the novel variational procedure or nonself-consistent approach.
  • Accurate DFT simulations were extended to molecular systems an order of magnitude larger than previously possible, including challenging condensed-phase systems.

Conclusions:

  • The developed LS-DFT methods offer a computationally efficient alternative for large-scale molecular simulations.
  • These methods significantly expand the scope of accurate DFT applications in chemistry and materials science.
  • The reduced computational cost facilitates broader adoption of advanced DFT calculations.