Download PDF by June Gunn Lee: Computational Materials Science: An Introduction, Second

By June Gunn Lee

This ebook covers the necessities of Computational technology and provides instruments and strategies to unravel fabrics technological know-how difficulties utilizing molecular dynamics (MD) and first-principles equipment. the recent variation expands upon the density practical conception (DFT) and the way the unique DFT has complex to a extra actual point via GGA+U and hybrid-functional equipment. It bargains 14 new labored examples within the LAMMPS, Quantum coffee, VASP and MedeA-VASP courses, together with computation of stress-strain habit of Si-CNT composite, mean-squared displacement (MSD) of ZrO2-Y2O3, band constitution and phonon spectra of silicon, and Mo-S battery method. It discusses tools as soon as thought of too pricey yet which are now reasonably priced. New examples additionally contain a number of post-processed effects utilizing VESTA, VMD, VTST, and MedeA.

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Extra resources for Computational Materials Science: An Introduction, Second Edition

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This algorithm is simple to implement, is time reversible and accurate, works well both for short and long timesteps, and is stable since positions and velocities are calculated for every timestep. It usually shows some energy fluctuations but no longtime energy drifts. 4 Predictor–corrector algorithm The predictor–corrector algorithm (Rahman 1964) is a higher-order algorithm that uses information of higher-order derivatives of the atom coordinates. It is also one of the most frequently implemented methods in MD.

14) where Z1 and Z2 are charges of the constituting atoms. 15) where C1 and C2 are constants. The second term for coulomb interaction is the long-range interaction that decays as 1 rij . 1) because the potential periodically accumulates and imposes a serious divergent problem. However, it can be efficiently dealt with by a technique called the Ewald sum (Ewald 1921). This method generates an artificial charge distribution localized around each ion twice: first with the opposite sign and next with the same sign as the ions (the magnitude is the same for both times).

Unstable (drifts or fluctuates too much), it is an indication of too large a timestep that overshoots the equilibrium positions. For atoms that move relatively fast due to high temperature, lighter mass, or steep potential curve, a shorter timestep is recommended. 4 Total simulation time A typical MD run may take 103–106 timesteps that correspond to total simulation time of only a few hundred nanoseconds (10 –9 s). Normally, this is sufficient to see usual static and dynamic properties in materials.

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