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In addition to the molecular force field, DL_POLY_2 allows the use of
an external force field. Examples of field available include:
- Electric field: (elec)
![\begin{displaymath}\mbox{$\underline{F_i}$} = \mbox{$\underline{F_i}$} + q_i. \mbox{$\underline{H}$} \end{displaymath}](img271.png) |
(2.107) |
- Oscillating shear: (oshm)
![\begin{displaymath}\mbox{$\underline{F}$}_{x}=A\cos(2n\pi.z/L_{z}) \end{displaymath}](img272.png) |
(2.108) |
- Continuous shear: (shrx)
![\begin{displaymath}
\mbox{$\underline{v}$}_{x}=\frac{1}{2}A\frac{\vert z\vert}{z}~~~~~~~~~~~~~:\vert z\vert>z_{0}\end{displaymath}](img273.png) |
(2.109) |
- Gravitational field: (grav)
![\begin{displaymath}\mbox{$\underline{F_i}$} = \mbox{$\underline{F_i}$} + m_i. \mbox{$\underline{H}$} \end{displaymath}](img274.png) |
(2.110) |
- Magnetic field: (magn)
![\begin{displaymath}\mbox{$\underline{F_i}$} = \mbox{$\underline{F_i}$} + q_i.(\mbox{$\underline{v_i}$}\wedge \mbox{$\underline{H}$})
\end{displaymath}](img275.png) |
(2.111) |
- Containing sphere: (sphr)
![\begin{displaymath}\mbox{$\underline{F}$}=A(R_{0}-r)^{-n}~~~~~~~~~~~~: r>R_{cut} \end{displaymath}](img276.png) |
(2.112) |
- Repulsive wall: (zbnd)
![\begin{displaymath}\mbox{$\underline{F}$}=A(z_{o}-z)~~~~~~~~~~~~: z>z_{o} \end{displaymath}](img277.png) |
(2.113) |
It is recommended that the use of an external field should be
accompanied by a thermostat (this does not apply to
examples 6 and 7, since these are conservative fields). The user is
advised to be careful with units!
In DL_POLY_2 external field forces are handled by the routine EXTNFLD.
Next: Long Ranged Electrostatic (Coulombic)
Up: The Intermolecular Potential Functions
Previous: Four Body Potentials
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W Smith
2003-05-12