2013
DOI: 10.1039/c3sm00062a
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Complexation between weakly basic dendrimers and linear polyelectrolytes: effects of grafts, chain stiffness, and pOH

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Cited by 9 publications
(16 citation statements)
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“…Whence, we only present the salient modifications to our earlier model to capture the physics of the system considered here. With respect to the framework outlined in ref , the following two additional free energy contributions arise for the model considered in the present article: The translational mixing entropies of the co- and counterions: β scriptF m i x = prefix∫ normald boldr .25em k { ρ k false( boldr false) false[ ln nobreak0em.25em⁡ ρ k ( r ) 1 + β μ k o false] } where ρ k ( r ) ( k = +,−) denotes the local density of the co- and counterions, μ k o represents the chemical potential of the k th species, and β = ( k B T ) −1 where k B denotes the Boltzmann constant. The free energy arising from electrostatic interactions: β scriptF e l e c = prefix∫ normald boldr .25em [ ρ e false( boldr false) Φ false( boldr false) + ε 8 π e 2 | Φ | 2 ] …”
Section: Theoretical Frameworkmentioning
confidence: 99%
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“…Whence, we only present the salient modifications to our earlier model to capture the physics of the system considered here. With respect to the framework outlined in ref , the following two additional free energy contributions arise for the model considered in the present article: The translational mixing entropies of the co- and counterions: β scriptF m i x = prefix∫ normald boldr .25em k { ρ k false( boldr false) false[ ln nobreak0em.25em⁡ ρ k ( r ) 1 + β μ k o false] } where ρ k ( r ) ( k = +,−) denotes the local density of the co- and counterions, μ k o represents the chemical potential of the k th species, and β = ( k B T ) −1 where k B denotes the Boltzmann constant. The free energy arising from electrostatic interactions: β scriptF e l e c = prefix∫ normald boldr .25em [ ρ e false( boldr false) Φ false( boldr false) + ε 8 π e 2 | Φ | 2 ] …”
Section: Theoretical Frameworkmentioning
confidence: 99%
“…The translational mixing entropies of the co- and counterions: β scriptF m i x = prefix∫ normald boldr .25em k { ρ k false( boldr false) false[ ln nobreak0em.25em⁡ ρ k ( r ) 1 + β μ k o false] } where ρ k ( r ) ( k = +,−) denotes the local density of the co- and counterions, μ k o represents the chemical potential of the k th species, and β = ( k B T ) −1 where k B denotes the Boltzmann constant.…”
Section: Theoretical Frameworkmentioning
confidence: 99%
“…Aptamers are polyelectrolytic in nature with their monomer units (nucleobases) participating in acid-base equilibrium and counterion binding reactions with the surrounding solution environments. Charge regulation and counterion binding in aptamers, or polyelectrolytes in general, are modulated by the metal ions present in the system, which can non-trivially alter their chemical and structural properties [8,9,10,11,12,13]. The presence of metal ions affects the performance of the aptamers as biosensing probes or therapeutics [14,15,16] due to the electrostatic screening of the charges on their surface, which changes their structure and chemistry.…”
Section: Introductionmentioning
confidence: 99%
“…However, accurate all-atom molecular dynamics (AAMD) simulations can only be applied routinely to fairly small dendrimer-DNA systems, 11,12 since AAMD simulations are computationally expensive. On the other hand, widely used coarse-grained (CG) models, [13][14][15][16] which use bead-spring or bead-rod chains to model dsDNA as an effectively single-strand linear polyelectrolyte, can simulate binding and wrapping of DNA around a dendrimer. However since the diameter of dsDNA is almost the same as the radius of the dendrimer, the double-helix structure of DNA might be critical for local arrangement of the DNA along the dendrimer surface and thereby strongly affect the structure of the dendrimer-DNA complex.…”
Section: Introductionmentioning
confidence: 99%