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Three-Body
Interactions These directives
are only use by a three-body run. BOHA
ILABEL is an integer label giving the index of the three-body bond type. The same label is used in the THBO directive. ILABEL must be 1 for the first three-body bond type, 2 for the second, and so on up to a maximum of MAXTHB. The analytic form of the potential is where is the bond angle in the crystal. is in eV , is in degrees. is a user defined equilibrium angle and is not necessarily the same as the actual bond angle in the crystal. For example, in quartz, the exact tetrahedral angle can be can be chosen for for the oxygen-silicon-oxygen bonds. However, the actual
angles in the crystal deviate slightly from equilibrium. There is a restriction
that none of the bond angles in the crystal can be 180 degrees (see QART).
The cutoff chosen is cos()
> - 0.999. Also the equilibrium angle supplied
must be greater than acos(0.999) and less than acos(-0.999). Printed outputTHREE BODY FORCE CONSTANT WITH INDEX ILABEL
THE FORM OF THE THREE BODY POTENTIAL IS V = 1/2*K3* (THETA - THETA0)**2
K3 = K3 THETA0 = THETA0 Error messagesERROR - A THREE BODY FORCE CONSTANT HAS BEEN DUPLICATEDThe integer ILABEL has already been used for another three-body bond. ERROR - THE EQUILIBRIUM BOND ANGLE MUST BE GREATER THAN ARCCOS(0.999)
ILABEL is an integer label giving the index of the three-body bond type (see BOHA). The analytic form of the potential is Where , and are the bond angles in the triangle of atoms i, j and k and , and are the bond lengths. is read in from the input record but not used. is in eV. There is no restriction on any of the bond angles being 180 degrees.Printed outputTHREE BODY FORCE CONSTANT WITH INDEX ILABEL
THE FORM OF THE THREE BODY POTENTIAL IS V = K3 * (1+3.0 * COS(THETAI) * COS(THETAJ) * COS(THETAK))/RIJ**3 * RIK**3 * RJK**3
K3 = K3 THETA0 = THETA0 Error messagesERROR - A THREE BODY FORCE CONSTANT HAS BEEN DUPLICATED The integer ILABEL has already been used for another three-body bond.
ILABEL is an integer label giving the index of the three-body bond type (see BOHA). The analytic form of the potential is Where is
the bond angle in the crystal. is
in eV ,
is
in degrees,
and
are in .
is a user defined equilibrium
angle and is not necessarily the same as the actual bond angle in the
crystal. and
are
the bond lengths from the central atom i to the two peripheral
atoms j and k, that is the angle .
Printed outputTHREE BODY FORCE CONSTANT WITH INDEX ILABEL
THE FORM OF THE THREE BODY POTENTIAL IS V = 1/2*K3* (THETA - THETA0)**2 * EXP(-R/RHO1) * EXP(-R/RHO2)
K3 = K3 RHO1 = RHO1 RHO2 = RHO2 Error messagesERROR - A THREE BODY FORCE CONSTANT HAS BEEN DUPLICATED
ILABEL is an integer label giving the index of the three-body bond type (see BOHA). The analytic form of the potential is
Printed outputTHREE BODY FORCE CONSTANT WITH INDEX ILABEL
THE FORM OF THE THREE BODY POTENTIAL IS V = 0.5* K3*(0.25*(THETA0-PI)**2-0.5*(THETA-PI)**2+0.25*((THETA-PI)**4) /((THETA0-PI)**2))
K3 = K3 THETA0 = THETA0 Error messagesERROR - A THREE BODY FORCE CONSTANT HAS BEEN DUPLICATED
ILABEL is an integer label giving the index of the three-body bond type (see BOHA). The analytic form of the potential is very complex, it is given below for the sake of completeness.
Where Where
is
the bond angle in the crystal,
is in eV ,
is
in degrees.
is a user defined equilibrium angle and is not necessarily the same
as the actual bond angle in the crystal. This potential may be used
when is
180 degrees, but not when
is 180 degrees (see BOHZ). It is designed
so that the second derivative of V with respect to is
the same as for BOHA
when .
Also the first derivative of V with respect to
tends to zero as tends
to .
This allows the derivative to be calculated using a power series approximation. Printed outputTHREE BODY FORCE CONSTANT WITH INDEX ILABEL
THE FORM OF THE THREE BODY POTENTIAL IS V = SIXTH ORDER POLYNOMIAL IN THETA WITH CORRECT LIMITS AT THETA = PI AND THETA = 0
K3 = K3 THETA0 = THETA0 Error message
ILABEL is an integer label giving the index of the three-body bond type (see BOHA). The analytic form of the potential is Where
is the bond angle in the crystal,
is in eV .
The equilibrium angle is .
This allows linear bonds to be treated. The derivatives are again calculated
using a power series if
is close to . Printed outputTHREE BODY FORCE CONSTANT WITH INDEX ILABEL
THE FORM OF THE THREE BODY POTENTIAL IS V = 1/2*K3* (THETA - PI)**2
K3 = K3 THETA0 = THETA0 Error messages
THRH
ILABEL is an integer label giving the index of the three-body bond type (see BOHA). The analytic form of the potential is Where
is in
eV .
is the
bond angle in the crystal. is
in degrees. is
a user defined equilibrium angle and is not necessarily the same as the
actual bond angle in the crystal. r01 and r02 are in
and are the equilibrium bond lengths of the ij and ik bonds
respectively.
ILABEL is an integer label giving the index of the three-body bond type (see BOHA). The analytic form of the potential is Where is in eV . r01 and r02 are in Å and are the equilibrium bond lengths of the ij and ik bonds respectively. |
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Next: Job Steps In DMAREL - Short Range Potential Input: Torsion Input Previous: Job Steps In DMAREL - Short Range Potential Input: Core-Shell Interactions Contents: Contents Page |