02090nas a2200181 4500008004100000022001400041245006700055210006700122260000900189300001100198490000800209520150000217100001701717700002401734700002501758700003401783856009101817 2021 eng d a0021-960600aEffective structure of a system with continuous polydispersity0 aEffective structure of a system with continuous polydispersity cJAN a0345030 v1543 a
In a system of N particles, with continuous size polydispersity, there exists an N(N - 1) number of partial structure factors, making it analytically less tractable. A common practice is to treat the system as an effective one component system, which is known to exhibit an artificial softening of the structure. The aim of this study is to describe the system in terms of M pseudospecies such that we can avoid this artificial softening but, at the same time, have a value of M << N. We use potential energy and pair excess entropy to estimate an optimum number of species, M-0. We then define the maximum width of polydispersity, Delta sigma (0), that can be treated as a monodisperse system. We show that M-0 depends on the degree and type of polydispersity and also on the nature of the interaction potential, whereas Delta sigma (0) weakly depends on the type of polydispersity but shows a stronger dependence on the type of interaction potential. Systems with a softer interaction potential have a higher tolerance with respect to polydispersity. Interestingly, M-0 is independent of system size, making this study more relevant for bigger systems. Our study reveals that even 1% polydispersity cannot be treated as an effective monodisperse system. Thus, while studying the role of polydispersity by using the structure of an effective one component system, care must be taken in decoupling the role of polydispersity from that of the artificial softening of the structure.
1 aPatel, Palak1 aNandi, Manoj, Kumar1 aNandi, Ujjwal, Kumar1 aBhattacharyya, Sarika, Maitra uhttp://library.ncl.res.in/content/effective-structure-system-continuous-polydispersity