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Madelung constant : ウィキペディア英語版
Madelung constant

The Madelung constant is used in determining the electrostatic potential of a single ion in a crystal by approximating the ions by point charges. It is named after Erwin Madelung, a German physicist.
Because the anions and cations in an ionic solid are attracting each other by virtue of their opposing charges, separating the ions requires a certain amount of energy. This energy must be given to the system in order to break the anion-cation bonds. The energy required to break these bonds for one mole of an ionic solid under standard conditions is the lattice energy.
== Formal expression ==
The Madelung constant shall allow for the calculation of the electric potential ''Vi'' of all ions of the lattice felt by the ion at position ''ri''
:V_i = \frac \sum_ \frac \sum_ \frac M_i
with M_i being the (dimensionless) Madelung constant of the ''i''th ion
:M_i = \sum_ \frac.
The electrostatic energy of the ion at site r_i then is the product of its charge with the potential acting at its site
:E_ = z_ieV_i = \frac z_i M_i.
There occur as many Madelung constants M_i in a crystal structure as ions occupy different lattice sites. For example, for the ionic crystal NaCl, there arise two Madelung constants – one for Na and another for Cl. Since both ions, however, occupy lattice sites of the same symmetry they both are of the same magnitude and differ only by sign. The electrical charge of the Na+ and Cl ion are assumed to be onefold positive and negative, respectively, z_=1 and z_=-1. The nearest neighbour distance amounts to half the lattice parameter of the cubic unit cell r_0=a/2 and the Madelung constants become
:M_\text=-M_\text = ^\prime \over .
The prime indicates that the term j=k=\ell=0 is to be left out. Since this sum is conditionally convergent it is not suitable as definition of Madelung's constant unless the order of summation is also specified. There are two "obvious" methods of summing this series, by expanding cubes or expanding spheres. The latter, though devoid of a meaningful physical interpretation (there are no spherical crystals) is rather popular because of its simplicity. Thus, the following expansion is often found in the literature:〔Charles Kittel: ''Introduction to Solid State Physics.'', Wiley 1995, ISBN 0-471-11181-3〕
:M = -6 +12/ \sqrt -8/ \sqrt +6/2 - 24/ \sqrt + \dotsb = -1.74756\dots.
However, this is wrong as this series diverges as was shown by Emersleben in 1951.〔O. Emersleben: ''Mathematische Nachrichten'' 4 (1951), 468〕〔D. Borwein, J. M. Borwein, K. F. Taylor: "Convergence of Lattice Sums and Madelung's Constant", ''J. Math. Phys.'' 26 (1985), 2999–3009, 〕 The summation over expanding cubes converges to the correct value. An unambiguous mathematical definition is given by Borwein, Borwein and Taylor by means of analytic continuation of an absolutely convergent series.
There are many practical methods for calculating Madelung's constant using either direct summation (for example, the Evjen method〔H. M. Evjen: "On the Stability of Certain Heteropolar Crystals", ''Phys. Rev.'' 39 (1932), 675–687, http://link.aps.org/abstract/PR/v39/p675〕) or integral transforms, which are used in the Ewald method.〔P. P. Ewald: "Die Berechnung optischer und elektrostatischer Gitterpotentiale", ''Ann. Phys.'' 64 (1921), 253–287, 〕

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