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root/OpenMD/trunk/samples/Madelung/quadrupoles/README.txt
Revision: 1921
Committed: Thu Aug 1 18:23:07 2013 UTC (12 years ago) by gezelter
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File size: 1851 byte(s)
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Fixed a few DumpWriter / FlucQ bugs.  Still working on Ewald, updated 
Quadrupolar test structures.

File Contents

# Content
1 This directory contains a set of quadrupolar crystals that can be used
2 to test electrostatic energies for quadrupole-quadrupole interactions.
3 The quadrupolar analogues to the structural Madelung constants for
4 ionic crystals were first worked out by Nagai and Nakamura who
5 computed the energies of certain selected quadrupole arrays and
6 obtained a number of these constants.[1] Their work is based on
7 earlier work on dipolar crystals that was done by Luttinger & Tisza
8 [2]. We have generated only the lowest energy configurations for the
9 linear quadrupoles
10
11 Lattice Quadrupole Direction Energy constants Notes
12 ------- -------------------- ---------------- ------
13 SC 111 -8.30 Fig 6a
14 BCC 011 -21.7 Fig 7b
15 FCC 111 -80.5 Fig 8
16
17 The electrostatic energy for one of these dipolar arrays is
18
19 E = C (3/4) N^2 Q^2
20
21 where C is the energy constant above, N is the number of quadrupoles
22 per unit volume, and Q is the strength of the dipole.
23
24 In the units used by OpenMD, with quadrupole moments of 1
25 Debye-angstrom, lengths in angstroms, and energies reported in
26 kcal / mol, the electrostatic energies are:
27
28 E = 14.39325 (3/4) C N^2 Q^2
29
30 E here is an energy density, so it must be multiplied by the total
31 volume of the box.
32
33
34 ---------------------------------------------------------------------
35 [1] O. Nagai and T. Nakamura, "Quadrupole Interaction in Crystals,"
36 Progress of Theoretical Physics 24 (2), 432-454 (1960)
37 doi: 10.1143/PTP.24.432, also see Errata: Progress of
38 Theoretical Physics 30 (3), 412 (1963). doi: 10.1143/PTP.30.412a
39
40 [2] J. M. Luttinger and L. Tisza, "Theory of Dipole Interaction in
41 Crystals," Phys. Rev. 70, 954–964 (1946) doi: 10.1103/PhysRev.70.954

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