Corrected SPH formulation 12 has been introduced in order to satisfy the
so-called consistency conditions:図 1.
図 2.
These equations insure that the integral approximation of a
function f coincides with f for constant and linear functions of space.
CSPH is a
correction of the kernel functions:図 3.
with
Where the parameters and are evaluated by enforcing the consistency condition, now given by the
point wise integration as:図 4.
図 5.
These equations enable the explicit evaluation of the correction
parameters and as:図 6.
図 7.
Since the evaluation of gradients of corrected kernel (which are
used for the SPH integration of continuum equations) becomes very expensive, corrected SPH
limited to order 0 consistency has been introduced. Therefore, the kernel correction reduces
to the following equations:図 8.
that is図 9.
図 10.
注: SPH corrections generally insure a better representation even if the
particles are not organized into a hexagonal compact net, especially close to the
integration domain frontiers. SPH corrections also allow the smoothing length to values different to the net size to be set.
1Bonet J., TSL Lok, Variational and Momentum Preservation Aspects of
Smooth Particle Hydrodynamic Formulations, Computer Methods in Applied
Mechanics and Engineering, Vol. 180, pp. 97-115 (1999).
2Bonet J. and Kulasegram S., Correction and Stabilization of Smooth
Particle Hydrodynamics Methods with Applications in Metal Forming
Simulations, Int. Journal Num. Methods in Engineering, Vol. 47, pp.
1189-1214, 2000.