Three-dimensional direct imaging of structural relaxation near the colloidal glass transition

From Soft-Matter
Jump to: navigation, search

Entry by Haifei Zhang, AP 225, Fall 2009

Soft matter keywords

Colloidal glasses, Relaxation, Supercooled fluid


Confocal microscopy was used to directly observe three-dimensional dynamics of particles in colloidal supercooled fluids and colloidal glasses. The fastest particles moved cooperatively; connected clusters of these mobile particles could be identiÞed; and the cluster size distribution, structure, and dynamics were investigated. The characteristic cluster size grew markedly in the supercooled ßuid as the glass transition was approached, in agreement with computer simulations; at the glass transition, however, there was a sudden drop in their size. The clusters of fast-moving particles were largest near the a-relaxation time scale for supercooled colloidal ßuids, but were also present, albeit with a markedly different nature, at shorter b-relaxation time scales, in both supercooled ßuid and glass colloidal phases.

Soft matter details

Do glasses flow?

When molten glass is cooled, it flows slower and slower, and at some point it's essentially solid. Unlike water, which is either water or ice, glass smoothly changes from a fluid to a really slow fluid to a glass. Why? The authors use small colloidal particles to model atoms in a glass; the authors look at them with a microscope. As the authors pack the particles together, if one of them wants to move, its neighbors have to cooperate. As they are packed even tighter, more of the particles have to cooperate for any to move. Perhaps when all of the particles in the sample have to cooperate, the sample is essentially a solid -- thus explaining what is happening with glass as it's cooled. This is a classic theory, and for the first time people can look at a real physical experiment and directly see cooperative motion by means of confocal microscope.

Most solid materials are crystals; the atoms are arranged in regular patterns.
Glass has no underlying regular structure. Instead, the atoms or molecules making up a glass are jumbled together.

Most solid materials are crystals; the atoms are arranged in regular patterns, for example, stacked like cannonballs as shown in the left picutre. The structure of crystals has been carefully studied for quite a long time, and is related to properties such as the strength of materials, their conductivity, how they break, and how they form.

Glass has no underlying regular structure. Instead, the atoms or molecules making up a glass are jumbled together, like the picture at right. They may be packed in so tightly they cannot move, but they are not packed in a regular way. Some materials naturally form glasses when they are cooled, such as silica (SiO2) (the primary chemical component of normal glass). What's weird is that structurally, glasses are the same as liquids -- if we just look at a microscopic snapshot of the position of the atoms, we can't tell the difference whereas it's really obvious that a crystal is something different from a liquid. So why is a glass a glass, and not a liquid? Or is it a liquid...?

When a glass-forming liquid is cooled, its viscosity increases -- it flows slower and slower. A simple definition of a glass is a liquid with a viscosity that is 10,000,000,000,000 times larger than the viscosity of water. This is somewhat arbitrary. In fact, a big question is, do glasses actually flow, or are they completely solid (infinite viscosity)? This has been extensively discussed on the internet; the authors believe that glasses do not flow any more than any other solid object flows.



A colloid is simply a fluid filled with lots of very small solid particles; this includes black ink, blood (filled with blood cells), and paint (filled with particles which stick to surfaces when they dry). Typically these particles are very small, between 1 nm and 1000 nm (one-millionth to one-thousandth of a millimeter). We use particles that are 0.002 mm in diameter, made from PMMA (the same material which is Plexiglas, if you have a much larger hunk of it). These particles basically act like marbles, that is, they ignore each other unless they bump into each other -- they don't have electric charges on them, for example.

Sometimes, our colloidal particles form crystalline arrays, like the picture at left, or the hexagons at right. These are similar in many ways to regular atomic crystals. In other cases, the colloidal particles pack close together in a random way, and form a colloidal glass; this is what is shown in some of the other pictures on this page. While normal atomic solids are formed by cooling, colloidal crystals and glasses are formed by cramming the particles together, usually by centrifuging them.

Confocal imaging


The authors use a confocal microscope to take 3D pictures of the samples, to see what the individual particles are doing as they move around in a colloidal glass. The authors can follow several thousand particles simultaneously, and watch their motion for several hours (sometimes several days). The authors look at how their motion changes when they are packed closer together, as the sample becomes a glass. Hopefully by understanding what occurs in a colloidal glass system, The authors can learn general properties of all glasses. The larger size of colloidal particles (as compared to atoms in regular glasses) make them possible to see, and it also means they move slower -- thus The authors don't need really fast electronics or techniques to see what they're doing.

The authors find that particles have to cooperate to move: if one particle can move a little ways, then one of its neighboring particles can move into the space left behind by the first particle; and then perhaps a third particle can follow the second particle, and so on. The more glass-like the sample is, the more particles cooperate at the same time. However, it takes longer and longer times before we see one of these cooperative events. Thus, it is possible that when all of the particles have to cooperate in order for any of them to move, you have a glass. Perhaps the time between cooperative rearrangements diverges, as well as the number of particles needed to cooperate, and it is the divergence of these two dyanamical quantities that distinguishes a glass from a liquid. Our data isn't inconsistent with this hypothesis -- which is a weasly scientist way of saying we have no idea if this really happens, but it's an intriguing idea that could be possible, so I mention it here on this web page. At least, the possibility is one reason why I find this interesting.

The figure on the right is from the experimental data, showing cooperative clusters of particles (the largest in this image is highlighted). All of the particles are actually the same size (the size of the large ones), the slower particles are made smaller so that the fast ones stand out.

Supercooled fluid V.S. Colloidal glasses


For a supercooled fluid, we have very large clusters of cooperative fast particles. This movie is from the sample that is closest to the glass transition, without actually being a glass.

For glasses, there are no large cooperative clusters. Since we're defining the fastest 5% of the particles as "fast", there is always some activity going on. However, it does not appear to involve many particles moving in a cooperative fashion as occurs for the liquid-like samples. Instead, there are small groups of particles which move slowly side-to-side, in somewhat of a cooperative fashion. This motion never results in large-scale rearrangements, unlike the supercooled fluids.


[1] Three-dimensional direct imaging of structural relaxation near the colloidal glass transition Weeks ER, Crocker JC, Levitt AC, et al., Science 287, 627 (2000).