International
Tables for
Crystallography
Volume B
Reciprocal space
Edited by U. Shmueli

International Tables for Crystallography (2010). Vol. B, ch. 3.4, pp. 456-457   | 1 | 2 |

## Section 3.4.12. Numerical illustrations

D. E. Williamsa

aDepartment of Chemistry, University of Louisville, Louisville, Kentucky 40292, USA

### 3.4.12. Numerical illustrations

| top | pdf |

Consider the case of the sodium chloride crystal structure (a face-centred cubic structure) as a simple example for evaluation of the Coulombic sum. The sodium ion can be taken at the origin, and the chloride ion halfway along an edge of the unit cell. The results can easily be generalized for this structure type by using the unit-cell edge length, a, as a scaling constant.

First, consider the nearest neighbours. Each sodium and each chloride ion is surrounded by six ions of opposite sign at a distance of . The Coulombic energy for the first coordination sphere is . Table 3.4.2.1 shows that the converged value of the lattice energy is . Thus the nearest-neighbour energy is over three times more negative than the total lattice energy. In the second coordination sphere each ion is surrounded by 12 similar ions at a distance of . The energy contribution of the second sphere is . Thus, major cancellation occurs and the net energy for the first two coordination spheres is which actually has the wrong sign for a stable crystal. The third coordination sphere again makes a negative contribution. Each ion is surrounded by eight ions of opposite sign at a distance of . The energy contribution is , now giving a total so far of . In the fourth coordination sphere each ion is surrounded by six others of the same sign at a distance of a. The energy contribution is +(1/2)(12)(1/a)(1389.3654) = +8336.19/a to yield a total of .

It is seen immediately by examining the numbers that the Coulombic sum is converging very slowly in direct space. Madelung (1918) devised a method for accurate evaluation of the sodium chloride lattice sum. However, his method is not generally applicable for more complex lattice structures. Evjen (1932) emphasized the importance of summing over a neutral domain, and replaced the sum with an integral outside of the first few shells of nearest neighbours. But the method of Ewald remained as the only completely general and accurate method of evaluating the Coulombic sum for a general lattice. Although it was derived in a somewhat different way, Ewald's method is equivalent to accelerated convergence for the special case of .

In the reciprocal lattice of sodium chloride only points with indices (hkl) all even or all odd are permitted by the face-centred symmetry. The reciprocal cell has edge length and the reciprocal-axis directions coincide with the direct-lattice axis directions. The closest points to the origin are the eight (111) forms at a distance of . For sodium chloride this distance is 0.3078 Å−1.

Table 3.4.12.1 shows the effect of convergence acceleration on the direct-space portion of the sum for the sodium chloride structure. The constant term is included in the values given. This constant term is always large if w is not zero; for instance, when this term is (Table 3.4.12.2). For the reciprocal-lattice sum is zero to six figures. Thus, only the direct sum (plus the constant term) is needed, evaluated out to 20 Å in direct space, to obtain six-figure accuracy. As shown in Table 3.4.2.1 above, the same summation effort without the use of accelerated convergence gave 8% error, or only slightly better than one-figure accuracy. The accelerated-convergence technique therefore yielded nearly five orders of magnitude improvement in accuracy, even without evaluation of the reciprocal-lattice sum.

 Table 3.4.12.1| top | pdf | Accelerated-convergence results for the Coulombic sum (n = 1) of sodium chloride (kJ mol−1, Å): the direct sum plus the constant term
Limitw = 0.1w = 0.15w = 0.2w = 0.3w = 0.4
6.0 −779.087 −838.145 −860.393 −924.275 −1125.372
8.0 −818.549 −860.194 −863.764 −924.282 −1125.372
10.0 −865.323 −862.818 −863.811 −924.282
12.0 −861.183 −862.824 −863.811
14.0 −862.717 −862.828
16.0 −862.792 −862.828
18.0 −862.810
20.0 −862.825
 Table 3.4.12.2| top | pdf | The reciprocal-lattice results (kJ mol−1, Å) for the Coulombic sum (n = 1) of sodium chloride
Limitw = 0.1w = 0.15w = 0.2w = 0.3w = 0.4
0.0 −277.872 −416.806 −555.742 −833.613 −1111.483
0.4 0.000 0.003 0.986 61.451 261.042
0.5   0.003 0.986 61.451 261.042
0.6       61.457 262.542
0.7       61.457 262.542
0.8         262.547
0.9         262.547

The column showing shows an example of how the reciprocal-lattice sum can also be neglected if lower accuracy is required. Table 3.4.12.2 shows that the reciprocal-lattice sum is still only 0.003. But now the direct-lattice sum only needs to be evaluated out to 14 Å, with further savings in calculation effort. For w values larger than 0.15 the reciprocal sum is needed. For this sum must be evaluated out to 0.8 Å−1 to obtain six-figure accuracy.

Table 3.4.12.3 illustrates an application for the dispersion sum. When five figures of accuracy can be obtained without consideration of the reciprocal sum. The direct sum is required out to 18 Å. If , better than four-figure accuracy can still be obtained without evaluating the reciprocal-lattice sum. In this case, the direct lattice needs to be summed only to 12 Å, and there is a saving of an order of magnitude in the length of the calculation. As with the Coulombic sum, if w is greater than 0.15 the reciprocal-lattice summation is needed; Table 3.4.12.4 shows the values.

 Table 3.4.12.3| top | pdf | Accelerated-convergence results for the dispersion sum (n = 6) of crystalline benzene (kJ mol−1, Å); the figures shown are the direct-lattice sum plus the two constant terms
Limitw = 0.1w = 0.15w = 0.2w = 0.3w = 0.4
6.0 −73.452 −77.761 −79.651 −61.866 76.645
8.0 −79.029 −80.374 −80.256 −61.870 76.645
10.0 −80.217 −80.571 −80.265 −61.870
12.0 −80.527 −80.585 −80.265
14.0 −80.578 −80.585
16.0 −80.588
18.0 −80.589
20.0 −80.589
 Table 3.4.12.4| top | pdf | The reciprocal-lattice results (kJ mol−1, Å) for the dispersion sum (n = 6) of crystalline benzene
Limitw = 0.1w = 0.15w = 0.2w = 0.3w = 0.4
0.0 −5.547 −16.706 −32.326 −43.681 80.947
0.3 0.000 −0.004 −0.321 −16.792 −117.106
0.4 0.000 −0.004 −0.324 −18.656 −152.651
0.5     −0.324 −18.716 −155.940
0.6       −18.719 −157.102
0.7       −18.719 −157.227
0.8         −157.233
0.9         −157.234
1.0         −157.234

The time required to obtain a lattice sum of given accuracy will vary depending on the particular structure considered and of course on the computer and program which are used. An example of timing for the benzene dispersion sum is given in Table 3.4.12.5 for the PCK83 program (Williams, 1984) running on a VAX-11/750 computer. In this particular case direct terms were evaluated at a rate of about 200 terms s−1 and reciprocal terms, being a sum themselves, were evaluated at a slower rate of about 5 terms s−1.

 Table 3.4.12.5| top | pdf | Approximate time (s) required to evaluate the dispersion sum (n = 6) for crystalline benzene within 0.001 kJ mol−1 truncation error
wDirect termsReciprocal termsTime, directTime, reciprocalTotal time
0.0 (not yet converged at 20 Å summation limit) >107
0.1 15904 0 77 0 77
0.15 4718 34 23 6 29
0.2 2631 78 13 14 27
0.3 1313 246 7 46 53
0.4 524 804 3 149 152

Table 3.4.12.5 shows the time required for evaluation of the dispersion sum using various values of the convergence constant, w. The timing figures show that there is an optimum choice for w; for the PCK83 program the optimum value indicated is 0.15–0.2 Å−1. In the program of Pietila & Rasmussen (1984) values in the range 0.15–0.2 Å−1 are also suggested. For the WMIN program (Busing, 1981) a slightly higher value of 0.25 Å−1 is suggested. Trial calculations can be used to determine the optimum value of w for the situation of a particular crystal structure, program and computer.

### References

Busing, W. R. (1981). WMIN, a computer program to model molecules and crystals in terms of potential energy functions. Oak Ridge National Laboratory Report ORNL-5747. Oak Ridge, Tennessee 37830, USA.
Evjen, H. M. (1932). The stability of certain heteropolar crystals. Phys. Rev. 39, 675–694.
Madelung, E. (1918). Das elektrische Feld in Systemen von regelmässig angeordneten Punktladungen. Phys. Z. 19, 524–532.
Pietila, L.-O. & Rasmussen, K. (1984). A program for calculation of crystal conformations of flexible molecules using convergence acceleration. J. Comput. Chem. 5, 252–260.
Williams, D. E. (1984). PCK83, a crystal molecular packing analysis program. Quantum Chemistry Program Exchange, Department of Chemistry, Indiana University, Bloomington, Indiana 47405, USA.