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ADVANCED USERS DMACRYS & NEIGHCRYS manual Manual ...

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molecules moving so their centres of mass within RDMA are now included in the higher multipole<br />

calculation. This aspect is a significant improvement on the original method for long molecules and small<br />

RDMA values (e.g. <strong>NEIGHCRYS</strong> default 15 Å).<br />

The spline is also applied to the electrostatic contributions calculated by Ewald summation. Hence the direct<br />

summation is out to the automatically determined direct summation limit + DSPL2, and differs from the true<br />

value by the difference between the true and spline values over the additional DSPL2 range. The cutoff<br />

value for the reciprocal lattice sum and the value of ETA are automatically adjusted to match the actual<br />

direct summation limit including DSPL2. The default accuracy of the Ewald summations means that the<br />

change in the Ewald summed terms is much smaller than the other terms.<br />

Currently <strong>NEIGHCRYS</strong>2.0.8 automatically adds the SPLI command.<br />

Printed output<br />

Potentials will be cutoff with a spline terminating at<br />

with limit in expansion set to splmax Angstroms<br />

splmin Angstroms<br />

Cut off value for direct lattice sum = CUTLAT lattice units<br />

Cut off value for reciprocal lattice sum = CUTRLT reciprocal lattice units<br />

Values of the constants used in these summations are:<br />

Eta parameter for division of sum between real and reciprocal lattice= HFCT0<br />

PI/(ETA^2 * Vol.Cell) = GFCT0<br />

Example output<br />

Potentials will be cutoff with a spline terminating at 2.00Angstroms<br />

with limit in expansion set to 4.00 Angstroms<br />

Cut off value for direct lattice sum = 1.901533 lattice units<br />

Cut off value for reciprocal lattice sum = 2.312667 reciprocal lattice units<br />

Values of the constants used in these summations are:<br />

Eta parameter for division of sum between real and reciprocal lattice= 1.954697<br />

PI/(ETA^2 * Vol.Cell) = 0.402803<br />

This change in the Ewald summation parameters is written out after the original data without a spline.<br />

3.6 POTENTIAL INPUT (other than multipoles & polarizabilities)<br />

3.6.1 REPULSION-DISPERSION POTENTIAL INPUT<br />

Operands<br />

None<br />

POTE<br />

This directive instructs the program to call the repulsion-dispersion potential input routine. This routine is<br />

menu driven with a menu of sub-directives. The sub-directives fall into seven classes: species data, repulsion<br />

& dispersion interactions, [core-shell interactions, three-body interactions, torsion interactions, restart subdirectives]<br />

and subroutine termination. Those in [] are not relevant to this version of <strong>DMACRYS</strong> but are<br />

retained for future use. Table 3.3 gives the sub-directives in each class.<br />

Table 3.3: DIRECTIVES FOR THE POTENTIAL INPUT SUBROUTINE<br />

Directive class<br />

Species data<br />

Repulsion-dispersion interactions<br />

Three-body interactions<br />

Four-body interactions<br />

The full list of potentials available is given in Appendix C.<br />

Directives<br />

SPEC, ENDS<br />

BUCK, MODI, LENN, MORS, BUC4, SPLP,<br />

MORQ, SPRI, COUL, VDWA, HULB, BUC7,<br />

NONE, BSPL,DBUC<br />

BOHA, TRID, MOLD, QART, SIXT, BOHZ,<br />

THRH, RRHA<br />

TOHA<br />

14

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