From leboeuf -A_T- CHIMCN.UMontreal.CA Fri Sep 30 19:16:10 1994 Received: from condor.CC.UMontreal.CA for leboeuf*- at -*CHIMCN.UMontreal.CA by www.ccl.net (8.6.9/930601.1506) id SAA07855; Fri, 30 Sep 1994 18:30:49 -0400 Received: from chims1.CHIMCN.UMontreal.CA by condor.CC.UMontreal.CA with SMTP id AA25724 (5.65c/IDA-1.4.4 for chemistry ^%at%^ ccl.net); Fri, 30 Sep 1994 18:29:46 -0400 Received: by chims1.CHIMCN.UMontreal.CA (930416.SGI/5.17) id AA28442; Fri, 30 Sep 94 18:28:33 -0400 From: leboeuf-: at :-CHIMCN.UMontreal.CA (Leboeuf Martin) Message-Id: <9409302228.AA28442*- at -*chims1.CHIMCN.UMontreal.CA> Subject: Re: multipole expansion To: chemistry- at -ccl.net Date: Fri, 30 Sep 1994 18:28:33 -0400 (EDT) Mime-Version: 1.0 Content-Type: text/plain; charset=US-ASCII Content-Transfer-Encoding: 7bit Content-Length: 1456 > From: hinsenk _-at-_)ERE.UMontreal.CA (Hinsen Konrad) > > ... > A multipole expansion is an expansion of the potential generated > by a spatially localized charge distribution for long distances. > Its convergence is guaranteed only outside a sphere containing > all the charges. To see if you can use multipole expansions > for molecular systems, draw a sphere around every molecule. > If any two spheres overlap, you are in trouble. In practice > this means that multipole expansions are useful only for > approximately spherical molecules, or for molecules in a > gas phase. > ... In other words, the multipole expansion (ME) is the solution of Laplace equation, which is why you have to be outside of the sphere containing the charge distribution. But recently, Koester et al. (JCP, 99 p1224 (1993)) developped a model for the solution of the Poisson equation. Since you are now solving Poisson's equation, there is no longer the restriction of being outside of your charge distribution. And in fact, we have implemented this scheme in our DFT code (deMon) and the molecular electrostatic potential calculated with this model has the right behavior both at long AND short distances from the molecules. And the computational effort is very similar to a ME calculation. Martin Leboeuf Departement de Chimie Universite de Montreal Montreal, Canada email: leboeuf:~at~:cerca.umontreal.ca