FRINK Linked Data Fragments server

Matches in SemOpenAlex for { <https://semopenalex.org/work/W2021832103> ?p ?o ?g. }

• W2021832103 endingPage "124903" @default.
• W2021832103 startingPage "124903" @default.
• W2021832103 abstract "A most promising off-lattice technique in order to simulate not only static but in addition dynamic behavior of linear and star-branched chains is the dissipative particle dynamics (DPD) method. In this model the atomistic representation of polymer molecules is replaced by a (coarse-grained) equivalent chain consisting of beads which are repulsive for each other in order to mimic the excluded volume effect (successive beads in addition are linked by springs). Likewise solvent molecules are combined to beads which in turn are repulsive for each other as well as for the polymer segments. The system is relaxed by molecular dynamics solving Newton's laws under the influence of short ranged conservative forces (i.e., repulsion between nonbonded beads and a proper balance of repulsion and attraction between bonded segments) and dissipative forces due to friction between particles, the latter representing the thermostat in conjunction with proper random forces. A variation of the strength of the repulsion between different types of beads allows the simulation of any desired thermodynamic situation. Static and dynamic properties of isolated linear and star-branched chains embedded in athermal, exothermal, and endothermal solvent are presented and theta conditions are examined. The generally accepted scaling concept for athermal systems is fairly well reproduced by linear and star-branched DPD chains and theta conditions appear for a unique parameter independent of functionality as in the case of Monte Carlo simulations. Furthermore, the correspondence between DPD and Monte Carlo data referring to the shape of chains and stars is fairly well, too. For dilute solutions the Zimm behavior is expected for dynamic properties which is indeed realized in DPD systems." @default.
• W2021832103 created "2016-06-24" @default.
• W2021832103 creator A5037029948 @default.
• W2021832103 creator A5081418489 @default.
• W2021832103 date "2009-09-28" @default.
• W2021832103 modified "2023-10-01" @default.
• W2021832103 title "Simulation of dilute solutions of linear and star-branched polymers by dissipative particle dynamics" @default.
• W2021832103 cites W1500828703 @default.
• W2021832103 cites W1634125899 @default.
• W2021832103 cites W1965752973 @default.
• W2021832103 cites W1966268897 @default.
• W2021832103 cites W1970763212 @default.
• W2021832103 cites W1970770365 @default.
• W2021832103 cites W1971729507 @default.
• W2021832103 cites W1972320957 @default.
• W2021832103 cites W1981410769 @default.
• W2021832103 cites W1982220212 @default.
• W2021832103 cites W1982854220 @default.
• W2021832103 cites W1988210656 @default.
• W2021832103 cites W1995062017 @default.
• W2021832103 cites W1996224306 @default.
• W2021832103 cites W1997293457 @default.
• W2021832103 cites W2009776840 @default.
• W2021832103 cites W2010087734 @default.
• W2021832103 cites W2011513455 @default.
• W2021832103 cites W2012556627 @default.
• W2021832103 cites W2012654776 @default.
• W2021832103 cites W2015145338 @default.
• W2021832103 cites W2017267092 @default.
• W2021832103 cites W2017591533 @default.
• W2021832103 cites W2018734438 @default.
• W2021832103 cites W2019299055 @default.
• W2021832103 cites W2019429499 @default.
• W2021832103 cites W2023873930 @default.
• W2021832103 cites W2025788547 @default.
• W2021832103 cites W2026782692 @default.
• W2021832103 cites W2032655419 @default.
• W2021832103 cites W2035128737 @default.
• W2021832103 cites W2044867956 @default.
• W2021832103 cites W2047412083 @default.
• W2021832103 cites W2048877789 @default.
• W2021832103 cites W2051147140 @default.
• W2021832103 cites W2051596663 @default.
• W2021832103 cites W2051893661 @default.
• W2021832103 cites W2052971487 @default.
• W2021832103 cites W2053055823 @default.
• W2021832103 cites W2053179595 @default.
• W2021832103 cites W2063922196 @default.
• W2021832103 cites W2064863523 @default.
• W2021832103 cites W2065052453 @default.
• W2021832103 cites W2070555488 @default.
• W2021832103 cites W2071452852 @default.
• W2021832103 cites W2074079250 @default.
• W2021832103 cites W2076274379 @default.
• W2021832103 cites W2077522575 @default.
• W2021832103 cites W2081203947 @default.
• W2021832103 cites W2084641108 @default.
• W2021832103 cites W2084782536 @default.
• W2021832103 cites W2085544727 @default.
• W2021832103 cites W2086043650 @default.
• W2021832103 cites W2087096169 @default.
• W2021832103 cites W2089005076 @default.
• W2021832103 cites W2089006288 @default.
• W2021832103 cites W2089580244 @default.
• W2021832103 cites W2089965878 @default.
• W2021832103 cites W2091071060 @default.
• W2021832103 cites W2091922856 @default.
• W2021832103 cites W2092441120 @default.
• W2021832103 cites W2093310284 @default.
• W2021832103 cites W2095213193 @default.
• W2021832103 cites W2097776558 @default.
• W2021832103 cites W2113447264 @default.
• W2021832103 cites W2129158276 @default.
• W2021832103 cites W2131487664 @default.
• W2021832103 cites W2148588891 @default.
• W2021832103 cites W2200932633 @default.
• W2021832103 cites W243433009 @default.
• W2021832103 cites W2963071818 @default.
• W2021832103 cites W3101050570 @default.
• W2021832103 cites W3106524745 @default.
• W2021832103 cites W4237795074 @default.
• W2021832103 cites W4241862909 @default.
• W2021832103 doi "https://doi.org/10.1063/1.3231854" @default.
• W2021832103 hasPubMedId "https://pubmed.ncbi.nlm.nih.gov/19791917" @default.
• W2021832103 hasPublicationYear "2009" @default.
• W2021832103 type Work @default.
• W2021832103 sameAs 2021832103 @default.
• W2021832103 citedByCount "35" @default.
• W2021832103 countsByYear W20218321032012 @default.
• W2021832103 countsByYear W20218321032014 @default.
• W2021832103 countsByYear W20218321032015 @default.
• W2021832103 countsByYear W20218321032016 @default.
• W2021832103 countsByYear W20218321032017 @default.
• W2021832103 countsByYear W20218321032018 @default.
• W2021832103 countsByYear W20218321032019 @default.
• W2021832103 countsByYear W20218321032020 @default.
• W2021832103 countsByYear W20218321032021 @default.
• W2021832103 countsByYear W20218321032022 @default.

• next