The diffusion of silica particles with radii ranging from 12 to 510 nm in dilute solutions of carboxymethyl cellulose (M w ؍ 180 to 1200 kg mol ؊1 , c CMC ؍ 5 to 1000 mg l ؊1 ) was investigated by means of dynamic light scattering at pH 5 in 0.01 mol l ؊1 NaCl. The viscosity of the polymer solut
A Simple Relation for the Concentration Dependence of Osmotic Pressure and Depletion Thickness in Polymer Solutions
✍ Scribed by Gerard J. Fleer; Alexander M. Skvortsov; Remco Tuinier
- Publisher
- John Wiley and Sons
- Year
- 2007
- Tongue
- English
- Weight
- 235 KB
- Volume
- 16
- Category
- Article
- ISSN
- 1022-1344
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✦ Synopsis
Abstract
We propose simple expressions $\Pi /\Pi _0 = 1 + (\varphi /\varphi _{{\rm ex}} )^{3\alpha - 1}$ and $(\delta _0 /\delta )^2 = 1 + (\varphi /\varphi _{{\rm ex}} )^{2\alpha }$ for the osmotic pressure Π and the depletion thickness δ as a function of the polymer concentration φ. Here, Π~0~ and δ~0~ correspond to the dilute limit, and φ~ex~ is an extrapolation concentration which is of the order of the overlap concentration φ~ov~. The De Gennes exponent α describes the concentration dependence of the semidilute correlation length $\xi \sim \varphi ^{ - \alpha }$; it is related to the Flory exponent ν through $\alpha = \nu /(3\nu - 1)$. The quantity φ~ex~ is experimentally accessible by extrapolating the semidilute limit towards Π = Π~0~ or δ = δ~0~. These expressions are exact in mean field, where the ratio φ~ex~/φ~ov~ (0.49 for Π, 0.41 for δ) follows from established models. For excluded‐volume chains they describe simulation data excellently: in this case φ~ex~/φ~ov~ is 0.69 for Π and again 0.41 for δ. We find also very good agreement with experimental data.
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