Difference between revisions of "Structural rearrangements that govern flow in colloidal glasses"

From Soft-Matter
Jump to: navigation, search
(Experiment)
Line 17: Line 17:
 
The use what appears to be a Maxwell-Boltzmann distribution to associate the frequency to the energy, temperature and shear modulus (<math>\mu</math>,) <math>ln(f(E)=\mu \frac{E}{\mu k_B T}</math>. Using this, the shear modulus is calculated to be one half of a value previously measured in a colloidal glass. The authors interpret this as confirmation that the oscillations in strain are thermally induced.  
 
The use what appears to be a Maxwell-Boltzmann distribution to associate the frequency to the energy, temperature and shear modulus (<math>\mu</math>,) <math>ln(f(E)=\mu \frac{E}{\mu k_B T}</math>. Using this, the shear modulus is calculated to be one half of a value previously measured in a colloidal glass. The authors interpret this as confirmation that the oscillations in strain are thermally induced.  
  
The thermally oscillations are necessarily reversible.
+
A key point is that the thermally oscillations aren't reversible and create rearrangements in the glass. The cumulative strain after twenty minutes was graphed for a vertical section of the glass. From, it is seen that localized regions of large strain persist and that these regions do not lead to macroscopic strain.
 +
[[Image:Cglass_cumstrain.png|thumb|Cumulative Strain.]]
 +
 
 +
The authors also applied positive shear strain which indicated that average displacement in y increased nearly linearly in z.
 +
[[Image:Cglass_linearstrain.png|thumb|Graph of strain in z versus y.]]
 +
The macroscopic shear strain was found to be <math>\gamma = 0.03</math> or <math>10^{-5}\frac{1}{s}</math>. The externally applied shear strain also produced localized regions of strain. Also there are regions where shear strain is opposite to the applied strain (blue).

Revision as of 03:56, 28 February 2009

Peter Schall, David A. Weitz, Frans Spaepen Science 318, 1895 (2007)

Soft Matter Keywords

Colloid, Glass

Abstract

Soft Matter Example

Experiment

The authors created a glass out of silica spheres <math>1.5 \mu m</math> radius spheres. The spheres were collected on a coverslip by centrifrugation at a packing faction of 0.61, which is higher than needed to created a glass and at a height of <math>42 \mu m</math>. A water-dimethylsulfoxide-fluorescein mixture was used to index match the spheres and then to contrast the spheres against the solvent. Then with the top stabilized, the coverslip at the bottom is sheared at rates about <math>10^{-5}s^{-1}</math>. The authors then recorded 3 Dimensional stacks using confocal microscopy.

Diagram of experimental setup.

The stacks revealed how the colloidal glass rearranged over the course of 20 minutes. The authors find that the strain is oscillatory, which they attribute to brownian motion. To confirm this, the authors analyze the glass in small cubic sections and measure the elastic energies. From this, they find that the distribution is exponential as indicated by the linearity of the semi-log graph in Figure 2.

Graph of relative frequency vs energy.

The use what appears to be a Maxwell-Boltzmann distribution to associate the frequency to the energy, temperature and shear modulus (<math>\mu</math>,) <math>ln(f(E)=\mu \frac{E}{\mu k_B T}</math>. Using this, the shear modulus is calculated to be one half of a value previously measured in a colloidal glass. The authors interpret this as confirmation that the oscillations in strain are thermally induced.

A key point is that the thermally oscillations aren't reversible and create rearrangements in the glass. The cumulative strain after twenty minutes was graphed for a vertical section of the glass. From, it is seen that localized regions of large strain persist and that these regions do not lead to macroscopic strain.

Cumulative Strain.

The authors also applied positive shear strain which indicated that average displacement in y increased nearly linearly in z.

Graph of strain in z versus y.

The macroscopic shear strain was found to be <math>\gamma = 0.03</math> or <math>10^{-5}\frac{1}{s}</math>. The externally applied shear strain also produced localized regions of strain. Also there are regions where shear strain is opposite to the applied strain (blue).