Effective charges along the melting line of colloidal crystals

The shear modulus G of charged colloidal crystals was measured at several constant particle densities n and varying salt concentrations c up to the melting salt concentration c M using torsional resonance spectroscopy. Far from the phase boundary the samples are polycrystalline and the shear modulus...

Ausführliche Beschreibung

Gespeichert in:
Bibliographische Detailangaben
Veröffentlicht in:The Journal of chemical physics 2006-11, Vol.125 (19), p.194714-194714-7
Hauptverfasser: Shapran, Larysa, Schöpe, Hans Joachim, Palberg, Thomas
Format: Artikel
Sprache:eng
Online-Zugang:Volltext
Tags: Tag hinzufügen
Keine Tags, Fügen Sie den ersten Tag hinzu!
Beschreibung
Zusammenfassung:The shear modulus G of charged colloidal crystals was measured at several constant particle densities n and varying salt concentrations c up to the melting salt concentration c M using torsional resonance spectroscopy. Far from the phase boundary the samples are polycrystalline and the shear modulus stays roughly constant as a function of c . Upon approaching the melting transition an increasing amount of wall based crystal material is formed surrounding a shrinking polycrystalline core and G drops nearly linearly. When the transition is complete G again stays constant. The morphologic transitions may be scaled upon a single master curve. For the polycrystalline morphology, the elastic data are evaluated in terms of a pairwise additive screened Coulomb interaction yielding a particle effective charge Z G * . Under de-ionized conditions Z 0 , G * is independent of n and significantly lower than expected from charge renormalization theory. With increasing salt concentration Z G * increases. The increase becomes more pronounced at larger n . By extrapolation we further obtain the melting line effective elasticity charge Z M , G * . Z M , G * shows a steplike increase with increasing n M and c M to values consistent with charge renormalization theory. Interestingly, the increase coincides semi-quantitatively with the one expected from the universal melting line for charged spheres, thus facilitating a consistent description of phase behavior and elasticity over an extended range of the phase diagram.
ISSN:0021-9606
1089-7690
DOI:10.1063/1.2395939