Matches in SemOpenAlex for { <https://semopenalex.org/work/W2321809398> ?p ?o ?g. }
- W2321809398 endingPage "263" @default.
- W2321809398 startingPage "256" @default.
- W2321809398 abstract "Abstract The structure and dynamics of polymers in confinements (such as porous media, channels and slits) depend not only on the characteristic length scales of the confinements but also on solvent types and interactions between polymers and confinement constituents. In this study, we show by performing both molecular dynamics (MD) and Langevin dynamics (LD) simulations that the lateral diffusion of a single flexible polymer in a good solvent in a slit should be determined by a complicated interplay among the slit height (H), solvent types and slit wall roughness. The slit wall roughness is tuned by employing either corrugated walls or smooth walls. We find from simulations that only when solvent molecules are implemented explicitly in MD simulations, the wall roughness makes a qualitative difference in the lateral diffusion coefficient ( D ∥ ) of the polymer: as H is decreased, D ∥ increases for smooth walls while D ∥ decreases for corrugated walls. Such a qualitative difference in D ∥ should be a solvent-mediated effect, which is not observed for implicit solvent models in LD simulations. The single polymer in the slit with the explicit solvent model follows Zimm dynamics while the polymer follows Rouse dynamics with the implicit solvent models. In the meantime, the wall roughness hardly affects the structure of the polymer in the slit. The density distribution functions of monomers ( ρ m ( z ) ) and solvent molecules ( ρ s ( z ) ) do not depend on whether the walls are corrugated or smooth. The radius of gyration ( R g ) is also insensitive to the wall roughness. On the other hand, the solvent model gives rise to a qualitative difference in ρ m ( z ) and R g , especially when the height (H) of the slit is small. For sufficiently small values of H, ρ m ( z ) depends on the size of solvent molecules used in the explicit solvent model. However, regardless of the solvent model and wall roughness, the scaling exponent (ν) of R g and the degree of polymerization (N) (i.e., R g ∼ N ν ) changes gradually from 0.6 to 0.75 as H decreases." @default.
- W2321809398 created "2016-06-24" @default.
- W2321809398 creator A5024538833 @default.
- W2321809398 creator A5047786018 @default.
- W2321809398 creator A5051996346 @default.
- W2321809398 date "2016-06-01" @default.
- W2321809398 modified "2023-09-27" @default.
- W2321809398 title "Effects of solvent and wall roughness on the dynamics and structure of a single polymer in a slit" @default.
- W2321809398 cites W1681493495 @default.
- W2321809398 cites W1942443447 @default.
- W2321809398 cites W1963652484 @default.
- W2321809398 cites W1964148794 @default.
- W2321809398 cites W1964460840 @default.
- W2321809398 cites W1975974197 @default.
- W2321809398 cites W1977087917 @default.
- W2321809398 cites W1978595244 @default.
- W2321809398 cites W1990316238 @default.
- W2321809398 cites W1995062017 @default.
- W2321809398 cites W1996224306 @default.
- W2321809398 cites W1999257160 @default.
- W2321809398 cites W2002576933 @default.
- W2321809398 cites W2005799666 @default.
- W2321809398 cites W2018703398 @default.
- W2321809398 cites W2020099077 @default.
- W2321809398 cites W2020438216 @default.
- W2321809398 cites W2031003731 @default.
- W2321809398 cites W2031405831 @default.
- W2321809398 cites W2041140088 @default.
- W2321809398 cites W2047188754 @default.
- W2321809398 cites W2048509789 @default.
- W2321809398 cites W2048717879 @default.
- W2321809398 cites W2054109073 @default.
- W2321809398 cites W2063391257 @default.
- W2321809398 cites W2069431751 @default.
- W2321809398 cites W2075723559 @default.
- W2321809398 cites W2084052818 @default.
- W2321809398 cites W2092991986 @default.
- W2321809398 cites W2101690798 @default.
- W2321809398 cites W2104965742 @default.
- W2321809398 cites W2117766669 @default.
- W2321809398 cites W2132619102 @default.
- W2321809398 cites W2136907935 @default.
- W2321809398 cites W2151561949 @default.
- W2321809398 cites W2164181486 @default.
- W2321809398 cites W2318802016 @default.
- W2321809398 cites W2318819237 @default.
- W2321809398 cites W2321801137 @default.
- W2321809398 cites W2327649503 @default.
- W2321809398 cites W3099588737 @default.
- W2321809398 cites W3105053316 @default.
- W2321809398 cites W3122490598 @default.
- W2321809398 cites W3123902762 @default.
- W2321809398 doi "https://doi.org/10.1016/j.polymer.2016.04.002" @default.
- W2321809398 hasPublicationYear "2016" @default.
- W2321809398 type Work @default.
- W2321809398 sameAs 2321809398 @default.
- W2321809398 citedByCount "4" @default.
- W2321809398 countsByYear W23218093982016 @default.
- W2321809398 countsByYear W23218093982019 @default.
- W2321809398 countsByYear W23218093982021 @default.
- W2321809398 crossrefType "journal-article" @default.
- W2321809398 hasAuthorship W2321809398A5024538833 @default.
- W2321809398 hasAuthorship W2321809398A5047786018 @default.
- W2321809398 hasAuthorship W2321809398A5051996346 @default.
- W2321809398 hasConcept C107365816 @default.
- W2321809398 hasConcept C120665830 @default.
- W2321809398 hasConcept C121332964 @default.
- W2321809398 hasConcept C126348684 @default.
- W2321809398 hasConcept C145912823 @default.
- W2321809398 hasConcept C159467904 @default.
- W2321809398 hasConcept C159985019 @default.
- W2321809398 hasConcept C178790620 @default.
- W2321809398 hasConcept C185592680 @default.
- W2321809398 hasConcept C188027245 @default.
- W2321809398 hasConcept C192562407 @default.
- W2321809398 hasConcept C199215989 @default.
- W2321809398 hasConcept C24890656 @default.
- W2321809398 hasConcept C2780471494 @default.
- W2321809398 hasConcept C521977710 @default.
- W2321809398 hasConcept C71039073 @default.
- W2321809398 hasConceptScore W2321809398C107365816 @default.
- W2321809398 hasConceptScore W2321809398C120665830 @default.
- W2321809398 hasConceptScore W2321809398C121332964 @default.
- W2321809398 hasConceptScore W2321809398C126348684 @default.
- W2321809398 hasConceptScore W2321809398C145912823 @default.
- W2321809398 hasConceptScore W2321809398C159467904 @default.
- W2321809398 hasConceptScore W2321809398C159985019 @default.
- W2321809398 hasConceptScore W2321809398C178790620 @default.
- W2321809398 hasConceptScore W2321809398C185592680 @default.
- W2321809398 hasConceptScore W2321809398C188027245 @default.
- W2321809398 hasConceptScore W2321809398C192562407 @default.
- W2321809398 hasConceptScore W2321809398C199215989 @default.
- W2321809398 hasConceptScore W2321809398C24890656 @default.
- W2321809398 hasConceptScore W2321809398C2780471494 @default.
- W2321809398 hasConceptScore W2321809398C521977710 @default.
- W2321809398 hasConceptScore W2321809398C71039073 @default.
- W2321809398 hasLocation W23218093981 @default.
- W2321809398 hasOpenAccess W2321809398 @default.