Interfacial water and ion distribution determine zeta potential and binding affinity of nanoparticles to biomolecules

The molecular features that dictate interactions between functionalized nanoparticles and biomolecules are not well understood. This is in part because for highly charged nanoparticles in solution, establishing a clear connection between the molecular features of surface ligands and common experimen...

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Veröffentlicht in:Nanoscale 2020-09, Vol.12 (35), p.18106-18123
Hauptverfasser: Liang, Dongyue, Dahal, Udaya, (Kelly) Zhang, Yongqian, Lochbaum, Christian, Ray, Dhiman, Hamers, Robert J., Pedersen, Joel A., Cui, Qiang
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container_end_page 18123
container_issue 35
container_start_page 18106
container_title Nanoscale
container_volume 12
creator Liang, Dongyue
Dahal, Udaya
(Kelly) Zhang, Yongqian
Lochbaum, Christian
Ray, Dhiman
Hamers, Robert J.
Pedersen, Joel A.
Cui, Qiang
description The molecular features that dictate interactions between functionalized nanoparticles and biomolecules are not well understood. This is in part because for highly charged nanoparticles in solution, establishing a clear connection between the molecular features of surface ligands and common experimental observables such as zeta potential requires going beyond the classical models based on continuum and mean field models. Motivated by these considerations, molecular dynamics simulations are used to probe the electrostatic properties of functionalized gold nanoparticles and their interaction with a charged peptide in salt solutions. Counterions are observed to screen the bare ligand charge to a significant degree even at the moderate salt concentration of 50 mM. As a result, the apparent charge density and zeta potential are largely insensitive to the bare ligand charge densities, which fall in the range of ligand densities typically measured experimentally for gold nanoparticles. While this screening effect was predicted by classical models such as the Manning condensation theory, the magnitudes of the apparent surface charge from microscopic simulations and mean-field models are significantly different. Moreover, our simulations found that the chemical features of the surface ligand (e.g., primaryvs.quaternary amines, heterogeneous ligand lengths) modulate the interfacial ion and water distributions and therefore the interfacial potential. The importance of interfacial water is further highlighted by the observation that introducing a fraction of hydrophobic ligands enhances the strength of electrostatic binding of the charged peptide. Finally, the simulations highlight that the electric double layer is perturbed upon binding interactions. As a result, it is the bare charge density rather than the apparent charge density or zeta potential that better correlates with binding affinity of the nanoparticle to a charged peptide. Overall, our study highlights the importance of molecular features of the nanoparticle/water interface and underscores a set of design rules for the modulation of electrostatic driven interactions at nano/bio interfaces.
doi_str_mv 10.1039/d0nr03792c
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While this screening effect was predicted by classical models such as the Manning condensation theory, the magnitudes of the apparent surface charge from microscopic simulations and mean-field models are significantly different. Moreover, our simulations found that the chemical features of the surface ligand (e.g., primaryvs.quaternary amines, heterogeneous ligand lengths) modulate the interfacial ion and water distributions and therefore the interfacial potential. The importance of interfacial water is further highlighted by the observation that introducing a fraction of hydrophobic ligands enhances the strength of electrostatic binding of the charged peptide. Finally, the simulations highlight that the electric double layer is perturbed upon binding interactions. As a result, it is the bare charge density rather than the apparent charge density or zeta potential that better correlates with binding affinity of the nanoparticle to a charged peptide. 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While this screening effect was predicted by classical models such as the Manning condensation theory, the magnitudes of the apparent surface charge from microscopic simulations and mean-field models are significantly different. Moreover, our simulations found that the chemical features of the surface ligand (e.g., primaryvs.quaternary amines, heterogeneous ligand lengths) modulate the interfacial ion and water distributions and therefore the interfacial potential. The importance of interfacial water is further highlighted by the observation that introducing a fraction of hydrophobic ligands enhances the strength of electrostatic binding of the charged peptide. Finally, the simulations highlight that the electric double layer is perturbed upon binding interactions. As a result, it is the bare charge density rather than the apparent charge density or zeta potential that better correlates with binding affinity of the nanoparticle to a charged peptide. 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This is in part because for highly charged nanoparticles in solution, establishing a clear connection between the molecular features of surface ligands and common experimental observables such as zeta potential requires going beyond the classical models based on continuum and mean field models. Motivated by these considerations, molecular dynamics simulations are used to probe the electrostatic properties of functionalized gold nanoparticles and their interaction with a charged peptide in salt solutions. Counterions are observed to screen the bare ligand charge to a significant degree even at the moderate salt concentration of 50 mM. As a result, the apparent charge density and zeta potential are largely insensitive to the bare ligand charge densities, which fall in the range of ligand densities typically measured experimentally for gold nanoparticles. While this screening effect was predicted by classical models such as the Manning condensation theory, the magnitudes of the apparent surface charge from microscopic simulations and mean-field models are significantly different. Moreover, our simulations found that the chemical features of the surface ligand (e.g., primaryvs.quaternary amines, heterogeneous ligand lengths) modulate the interfacial ion and water distributions and therefore the interfacial potential. The importance of interfacial water is further highlighted by the observation that introducing a fraction of hydrophobic ligands enhances the strength of electrostatic binding of the charged peptide. Finally, the simulations highlight that the electric double layer is perturbed upon binding interactions. As a result, it is the bare charge density rather than the apparent charge density or zeta potential that better correlates with binding affinity of the nanoparticle to a charged peptide. Overall, our study highlights the importance of molecular features of the nanoparticle/water interface and underscores a set of design rules for the modulation of electrostatic driven interactions at nano/bio interfaces.</abstract><cop>CAMBRIDGE</cop><pub>Royal Soc Chemistry</pub><pmid>32852025</pmid><doi>10.1039/d0nr03792c</doi><tpages>18</tpages><orcidid>https://orcid.org/0000-0002-3918-1860</orcidid><orcidid>https://orcid.org/0000-0003-3821-9625</orcidid><orcidid>https://orcid.org/0000-0002-7103-0886</orcidid><orcidid>https://orcid.org/0000-0001-6214-5211</orcidid></addata></record>
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subjects Affinity
Amines
Binding
Biomolecules
Charge density
Charge simulation
Chemistry
Chemistry, Multidisciplinary
Computer simulation
Diamonds
Electric double layer
Free energy
Gold
Ion distribution
Ligands
Materials Science
Materials Science, Multidisciplinary
Metal Nanoparticles
Molecular dynamics
Molecular Dynamics Simulation
Nanoparticles
Nanoscience & Nanotechnology
Nanostructure
Peptides
Physical Sciences
Physics
Physics, Applied
Protonation
Quaternary ammonium salts
Saline solutions
Science & Technology
Science & Technology - Other Topics
Simulation
Static Electricity
Surface charge
Surface Properties
Technology
Water
title Interfacial water and ion distribution determine zeta potential and binding affinity of nanoparticles to biomolecules
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