Failure of Debye-Hückel Screening in Low-Charge Colloidal Suspensions

Derjaguin–Landau–Verwey–Overbeek (DLVO) theory remains the cornerstone of colloid stability. Electrostatic interactions dominate van der Waals attractions at large colloid-colloid separations h, unless strongly screened. Under these conditions, the potential U ( h )...

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Main Authors: Franceska Waggett, Mohamad Danial Shafiq, Paul Bartlett
Format: Article
Language:English
Published: MDPI AG 2018-10-01
Series:Colloids and Interfaces
Subjects:
Online Access:http://www.mdpi.com/2504-5377/2/4/51
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spelling doaj-e79b4fe4c76847d7971e0227cfe8d21f2020-11-24T21:00:31ZengMDPI AGColloids and Interfaces2504-53772018-10-01245110.3390/colloids2040051colloids2040051Failure of Debye-Hückel Screening in Low-Charge Colloidal SuspensionsFranceska Waggett0Mohamad Danial Shafiq1Paul Bartlett2School of Chemistry, University of Bristol, Bristol BS8 1TS, UKSchool of Chemistry, University of Bristol, Bristol BS8 1TS, UKSchool of Chemistry, University of Bristol, Bristol BS8 1TS, UKDerjaguin–Landau–Verwey–Overbeek (DLVO) theory remains the cornerstone of colloid stability. Electrostatic interactions dominate van der Waals attractions at large colloid-colloid separations h, unless strongly screened. Under these conditions, the potential U ( h ) between charged colloids is expected to be exponentially screened, U ( h ) ∼ exp ( − κ h ) / h , with κ − 1 = λ D where λ D is the classical Debye-Hückel screening length. By measuring the force between individual charged particles at dilute electrolyte concentrations (<mM) using optical tweezers, we tested experimentally the prediction κ − 1 = λ D in a nonpolar solvent. At low salt concentrations, we found close agreement between the directly-measured decay length κ − 1 and Debye-Hückel predictions. However, above a critical electrolyte concentration (≈450 μ M), we obtained significant discrepancies between measured and predicted screening lengths, with κ − 1 ≫ λ D . In marked contrast to expectations, we found that the measured screening length κ − 1 appears to grow as the ionic strength of the solution is increased. The origin of this discrepancy is discussed and the importance of considering the surface is highlighted.http://www.mdpi.com/2504-5377/2/4/51electrostaticsDLVOoptical manipulation
collection DOAJ
language English
format Article
sources DOAJ
author Franceska Waggett
Mohamad Danial Shafiq
Paul Bartlett
spellingShingle Franceska Waggett
Mohamad Danial Shafiq
Paul Bartlett
Failure of Debye-Hückel Screening in Low-Charge Colloidal Suspensions
Colloids and Interfaces
electrostatics
DLVO
optical manipulation
author_facet Franceska Waggett
Mohamad Danial Shafiq
Paul Bartlett
author_sort Franceska Waggett
title Failure of Debye-Hückel Screening in Low-Charge Colloidal Suspensions
title_short Failure of Debye-Hückel Screening in Low-Charge Colloidal Suspensions
title_full Failure of Debye-Hückel Screening in Low-Charge Colloidal Suspensions
title_fullStr Failure of Debye-Hückel Screening in Low-Charge Colloidal Suspensions
title_full_unstemmed Failure of Debye-Hückel Screening in Low-Charge Colloidal Suspensions
title_sort failure of debye-hückel screening in low-charge colloidal suspensions
publisher MDPI AG
series Colloids and Interfaces
issn 2504-5377
publishDate 2018-10-01
description Derjaguin–Landau–Verwey–Overbeek (DLVO) theory remains the cornerstone of colloid stability. Electrostatic interactions dominate van der Waals attractions at large colloid-colloid separations h, unless strongly screened. Under these conditions, the potential U ( h ) between charged colloids is expected to be exponentially screened, U ( h ) ∼ exp ( − κ h ) / h , with κ − 1 = λ D where λ D is the classical Debye-Hückel screening length. By measuring the force between individual charged particles at dilute electrolyte concentrations (<mM) using optical tweezers, we tested experimentally the prediction κ − 1 = λ D in a nonpolar solvent. At low salt concentrations, we found close agreement between the directly-measured decay length κ − 1 and Debye-Hückel predictions. However, above a critical electrolyte concentration (≈450 μ M), we obtained significant discrepancies between measured and predicted screening lengths, with κ − 1 ≫ λ D . In marked contrast to expectations, we found that the measured screening length κ − 1 appears to grow as the ionic strength of the solution is increased. The origin of this discrepancy is discussed and the importance of considering the surface is highlighted.
topic electrostatics
DLVO
optical manipulation
url http://www.mdpi.com/2504-5377/2/4/51
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