Understanding the fundamental properties of polymeric liquids remains a challenge in materials science and soft matter physics. Here, we present a simple and computationally efficient criterion for topological constraints, i.e., uncrossability of chains, in polymeric liquids using the dissipative particle dynamics (DPD) method. No new length scales or forces are added. To demonstrate that this approach really prevents chain crossings, we study a melt of linear homopolymers. We show that for short chains the model correctly reproduces Rouse-like dynamics whereas for longer chains the dynamics becomes reptational as the chain length is increased—something that is not attainable using standard DPD or other coarse-grained soft potential methods
This thesis focuses on the investigation of models of locally stiff polymers in the melt by means of...
We model high molecular weight homopolymers in semidilute concentration via Dissipative Particle Dyn...
We study the diffusive motion of a (non-selfinteracting) chain through a quenched random environment...
Understanding the fundamental properties of polymeric liquids remains a challenge in materials scien...
We introduce a framework for model reduction of polymer chain models for dissipative particle dynami...
An important feature of a melt of long polymers is that the bonds of the chains cannot cross each ot...
We present here a systematic study of dynamic behavior for polymer (PE) melt by means of Dissipativ...
A new technique, dissipative particle dynamics (DPD), appears promising as a means of studying the d...
We present coarse-grained molecular dynamics simulations of poly(ethylene-alt-propylene) (PEP) melts...
AbstractWe model high molecular weight homopolymers in semidilute concentration via Dissipative Part...
A full inspection of the motion and relaxation of soft matter systems, such as polymer melts, soluti...
The influence of uncrossability constraints on the dynamics of coarse-grained polymer melts was stud...
Over the past half century, molecular dynamics simulation techniques have advanced considerably, aim...
We analyse the knotting behaviour of linear polymer melts in two types of soft-core models, namely d...
ABSTRACT: We use molecular dynamics simulations of the Kremer− Grest (KG) bead−spring model of polym...
This thesis focuses on the investigation of models of locally stiff polymers in the melt by means of...
We model high molecular weight homopolymers in semidilute concentration via Dissipative Particle Dyn...
We study the diffusive motion of a (non-selfinteracting) chain through a quenched random environment...
Understanding the fundamental properties of polymeric liquids remains a challenge in materials scien...
We introduce a framework for model reduction of polymer chain models for dissipative particle dynami...
An important feature of a melt of long polymers is that the bonds of the chains cannot cross each ot...
We present here a systematic study of dynamic behavior for polymer (PE) melt by means of Dissipativ...
A new technique, dissipative particle dynamics (DPD), appears promising as a means of studying the d...
We present coarse-grained molecular dynamics simulations of poly(ethylene-alt-propylene) (PEP) melts...
AbstractWe model high molecular weight homopolymers in semidilute concentration via Dissipative Part...
A full inspection of the motion and relaxation of soft matter systems, such as polymer melts, soluti...
The influence of uncrossability constraints on the dynamics of coarse-grained polymer melts was stud...
Over the past half century, molecular dynamics simulation techniques have advanced considerably, aim...
We analyse the knotting behaviour of linear polymer melts in two types of soft-core models, namely d...
ABSTRACT: We use molecular dynamics simulations of the Kremer− Grest (KG) bead−spring model of polym...
This thesis focuses on the investigation of models of locally stiff polymers in the melt by means of...
We model high molecular weight homopolymers in semidilute concentration via Dissipative Particle Dyn...
We study the diffusive motion of a (non-selfinteracting) chain through a quenched random environment...