Difference between revisions of "Does size matter? Elasticity of compressed suspensions of colloidal- and granular-scale microgels"

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Figure 2 shows the Storage Modulus G' and Loss Modulus G'' as a function of oscillatory frequency. G' is nearly constant across all frequency ranges and increases with crosslink density. Indicating that the degree of networking in the microgel is the only discriminating factor in G'. If G' is dependent solely on crosslink density, G' should be independent of particle size. Normalizing all of the data according to average length of the elastically active chains such that all the G' data can be plotted on the same plot shows this is indeed the case. The dashed line in Figure 3 shows the normalized G' expected for macrogels. As stress increases, the microgel deforms, and approaches the predicted normalized G' value for macrogels. This demonstrates that at low polymer concentration, when the particles are free to move in response to an applied stress, relaxation is attained by particulate rearrangement; however, at high pressures when particulate rearrangement is not possible, microgel shear response is nearly identical to behavior predicted by macrogel models.  
 
Figure 2 shows the Storage Modulus G' and Loss Modulus G'' as a function of oscillatory frequency. G' is nearly constant across all frequency ranges and increases with crosslink density. Indicating that the degree of networking in the microgel is the only discriminating factor in G'. If G' is dependent solely on crosslink density, G' should be independent of particle size. Normalizing all of the data according to average length of the elastically active chains such that all the G' data can be plotted on the same plot shows this is indeed the case. The dashed line in Figure 3 shows the normalized G' expected for macrogels. As stress increases, the microgel deforms, and approaches the predicted normalized G' value for macrogels. This demonstrates that at low polymer concentration, when the particles are free to move in response to an applied stress, relaxation is attained by particulate rearrangement; however, at high pressures when particulate rearrangement is not possible, microgel shear response is nearly identical to behavior predicted by macrogel models.  
  
The loss modulus behavior in Figure 2 can also be explained according competing dissipation mechanisms. At low frequencies, stress is readily dissipated by particulate shearing, leading to large losses. This is shown by the definitive minimum attained in the middle frequency range. As frequency increases, dissipation is limited to the viscous regime of solvent moving past the particles rather than particle-particle dissipation. The rapid oscillation kintically limits particulate motion, leading to increased G''.
+
The loss modulus behavior in Figure 2 can also be explained according competing dissipation mechanisms. At low frequencies, stress is readily dissipated by particulate shearing, leading to large losses. This is shown by the definitive minimum attained in the middle frequency range. As frequency increases, dissipation is limited to the viscous regime of solvent moving past the particles rather than particle-particle dissipation. The rapid oscillation kinetically limits particulate motion, leading to increased G''.

Revision as of 20:38, 21 September 2012

Currently Being Edited by Joseph

Introduction

Microgels are particles consisting of a cross-linked polymer network swollen with solvent. Most colloids consist of incompressible solids suspended in solution, whereas microgels can be compressed and deformed. The degree of microgel deformation is governed by the cross-link density of the polymer network. Due to their compressibility, microgels can achieve much higher packing densities (jammed packing) compared to the hard spheres inherent to many typical colloidal solutions. When microgel particles become jammed, they are unable to rearrange in response to an applied stress, giving rise to an effective glass transition. However, it has been noted that thermally induced particle rearrangement can occur in these systems. It is difficult to describe the nature of these interactions because particle properties are not easily isolated from interparticle interactions.

In an effort to elucidate the thermal effects on elasticity of microgels, the author explores the elasticity and rheology of colloidal and granular microgels. By comparing microgels of widely varying sizes the effects of interparticle interactions can be accounted for. Due to the small size of colloidal microgels, Brownian interactions play a significant role in the stress response in the particle - hence their stress response will be a combination of intraparticle and interparticle interactions. However, for the larger granular microgels, it is hypothesized that Brownian interactions will play a negligible role in the stress response, eliminating the interparticle component of the stress response. By comparing the stress response of the colloidal microgels to the granular microgels in both compression and shear, the stress responses arising from intraparticle and interparticle interactions will be separated and evaluated.


Experimental

Colloidal microgels where made of poly(N-isopropylacrylamide-co-acrylic acid) (p(NIPAAm-co-AAc)) via precipiation polymerization. Three different cross-link densities were created in the microgels - 0.1, 1.0, and 10 wt% relative to monomer concentration. Granular microgels were made from p(NIPAAm-co-AAc) as well, except particle size was maintained between 100-400 microns via emulsion polymerization. A second type of granular microgel of similar size was made from polyacrylamide again via emulsion polymerization.

Isotropic compression was performed on the colloidal and granular microgels by way of osmostic pressure. The microgels were emmersed in a solution of polyethylene glycol (PEG) of known osmotic pressure and stressed between 1-200kPa. Shear stress was inflicted on all specimen types via a plate-plate rheometer.

Effect of Particle Size on Compressibility

The osmotic pressure for a macrogel is described by Flory–Rehner theory: <math>pi=pim+pie</math>, where pi is the total osmotic pressure, pim is the osmotic pressure due to mixing and pie is the osmotic pressure due to elastic contributions of the gel matrix.

As the particles are compressed by the applied pressure, the particles become squeezed together, forming a tightly packed network. As the network compresses, the elastic contribution to osmotic pressure dominates the Flory-Rehner equation giving rise to the sharp increase in osmotic pressure for low polymer concentrations. However, as the pressure is increased further, the polymer matrix becomes fully compressed, and the only way for the matrix to further contract is through the expulsion of entrapped solvent (raising the polymer concentration). As the solvent escapes the gel matrix and begins to mix with the rest polymer of the polymer, the osmotic pressure contribution as a result of mixing increases. Thus, at high polymer concentration when the polymer is fully compressed, the elastic contribution to osmotic pressure is negligible and the Flory-Rehner equation is dominated by the mixing term.

Based on this reasoning, all microgels regardless of size, should behave similarly for a given cross-link density. Moreover, while the elastic contributions to osmotic pressure will differ for small polymer concentrations in the elastic regime, all microgels should converge to a singular concentration-osmotic pressure relationship in the mixing regime. From Figure 1, we see this is indeed the case. From Figure 1, we can conclude that microgels follow similar principles as macrogels when subjected to hydrostatic pressure.

Effect of Particle Size on Shear Response

Figure 2 shows the Storage Modulus G' and Loss Modulus G as a function of oscillatory frequency. G' is nearly constant across all frequency ranges and increases with crosslink density. Indicating that the degree of networking in the microgel is the only discriminating factor in G'. If G' is dependent solely on crosslink density, G' should be independent of particle size. Normalizing all of the data according to average length of the elastically active chains such that all the G' data can be plotted on the same plot shows this is indeed the case. The dashed line in Figure 3 shows the normalized G' expected for macrogels. As stress increases, the microgel deforms, and approaches the predicted normalized G' value for macrogels. This demonstrates that at low polymer concentration, when the particles are free to move in response to an applied stress, relaxation is attained by particulate rearrangement; however, at high pressures when particulate rearrangement is not possible, microgel shear response is nearly identical to behavior predicted by macrogel models.

The loss modulus behavior in Figure 2 can also be explained according competing dissipation mechanisms. At low frequencies, stress is readily dissipated by particulate shearing, leading to large losses. This is shown by the definitive minimum attained in the middle frequency range. As frequency increases, dissipation is limited to the viscous regime of solvent moving past the particles rather than particle-particle dissipation. The rapid oscillation kinetically limits particulate motion, leading to increased G.