Ewald sum: Difference between revisions

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The '''Ewald sum''' technique <ref>[http://dx.doi.org/10.1002/andp.19213690304  Paul Ewald "Die Berechnung Optischer und Electrostatischer Gitterpotentiale", Annalen der Physik '''64''' pp. 253-287 (1921)]</ref>  is widely used in order to simulate systems with
The '''Ewald sum''' technique <ref>[http://dx.doi.org/10.1002/andp.19213690304  Paul Ewald "Die Berechnung Optischer und Electrostatischer Gitterpotentiale", Annalen der Physik '''64''' pp. 253-287 (1921)]</ref>  is widely used in order to simulate systems with
[[long range interactions]] (typically, [[Electrostatics |electrostatic interactions]]). Its aim is the computation of the interaction of a system with [[periodic boundary conditions]] with all its replicas. This is accomplished by the introduction of fictitious "charge clouds" that shield the charges. The interaction is then divided into a shielded part, which may be evaluated by the usual means, and a part that cancels the introduction of the clouds, which is evaluated in [[Fourier_analysis | Fourier space]].
[[long range interactions]] (typically, [[Electrostatics |electrostatic interactions]]). Its aim is the computation of the interaction of a system with [[periodic boundary conditions]] with all its replicas. This is accomplished by the introduction of fictitious "charge clouds" that shield the charges. The interaction is then divided into a shielded part, which may be evaluated by the usual means, and a part that cancels the introduction of the clouds, which is evaluated in [[Fourier_analysis | Fourier space]].
==Particle mesh==
==Particle mesh==
*[http://dx.doi.org/10.1063/1.464397    Tom Darden, Darrin York, and Lee Pedersen "Particle mesh Ewald: An N·log(N) method for Ewald sums in large systems", Journal of Chemical Physics '''98''' pp. 10089-10092 (1993)]
<ref>[http://dx.doi.org/10.1063/1.464397    Tom Darden, Darrin York, and Lee Pedersen "Particle mesh Ewald: An N·log(N) method for Ewald sums in large systems", Journal of Chemical Physics '''98''' pp. 10089-10092 (1993)]</ref>
====Smooth particle mesh (SPME)====
====Smooth particle mesh (SPME)====
*[http://dx.doi.org/10.1063/1.470117    Ulrich Essmann, Lalith Perera,  Max L. Berkowitz,    Tom Darden, Hsing Lee, and Lee G. Pedersen "A smooth particle mesh Ewald method", Journal of Chemical Physics '''103''' pp. 8577-8593  (1995)]
<ref>[http://dx.doi.org/10.1063/1.470117    Ulrich Essmann, Lalith Perera,  Max L. Berkowitz,    Tom Darden, Hsing Lee, and Lee G. Pedersen "A smooth particle mesh Ewald method", Journal of Chemical Physics '''103''' pp. 8577-8593  (1995)]</ref>
*[http://dx.doi.org/10.1063/1.3446812  Han Wang, Florian Dommert, and Christian Holm "Optimizing working parameters of the smooth particle mesh Ewald algorithm in terms of accuracy and efficiency", Journal of Chemical Physics '''133''' 034117 (2010)]
<ref>[http://dx.doi.org/10.1063/1.3446812  Han Wang, Florian Dommert, and Christian Holm "Optimizing working parameters of the smooth particle mesh Ewald algorithm in terms of accuracy and efficiency", Journal of Chemical Physics '''133''' 034117 (2010)]</ref>
 
==See also==
==Related pages==
*[[Reaction field]]
*[[Reaction field]]
==References==
==References==

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The Ewald sum technique [1] is widely used in order to simulate systems with long range interactions (typically, electrostatic interactions). Its aim is the computation of the interaction of a system with periodic boundary conditions with all its replicas. This is accomplished by the introduction of fictitious "charge clouds" that shield the charges. The interaction is then divided into a shielded part, which may be evaluated by the usual means, and a part that cancels the introduction of the clouds, which is evaluated in Fourier space.

Particle mesh

[2]

Smooth particle mesh (SPME)

[3] [4]

See also

References

Related reading

External resources