All matter consists of one or more phases — regions of space with uniform structure and physical properties. Everyone is familiar with the common phases of H2O (solid, liquid, and gas), also known as ice, water, and steam. Similarly, polymeric materials can form a variety of different solid or liquid phases that determine their properties and ultimate utility. This is especially true of block copolymers, the highly useful self-assembling macromolecules created when a polymer chain of one type (call it “Block A”) is chemically connected with a polymer chain of a different type (“Block B”).
“If you want a block copolymer that has a certain property, you pick the right phase for a given application of interest,” says Chris Bates, assistant professor in the Materials Department at the UC Santa Barbara College of Engineering. “For the rubber in shoes, you want one phase; to make a membrane, you want a different one.”
Only about five phases have been discovered in the simplest block copolymers. Finding a new phase is rare, but Bates and a team of UCSB researchers including Professor Glenn Fredrickson (chemical engineering), Professor Craig Hawker (materials), Morgan Bates, a staff scientist and the assistant director for technology at the Dow Materials Institute at UCSB, and Joshua Lequieu, a postdoctoral researcher with Fredrickson, have done just that. They describe their findings in an article titled "Stability of the A15 Phase in Diblock Copolymer Melts" and published in the July 2 issue of the Proceedings of the National Academy of Sciences.
About 12 months ago, Morgan Bates was doing some experimental work on polymers she had synthesized in the lab. “We wanted to understand the fundamental parameters that govern self-assembly of block copolymers by examining what happens when you tweak block chemistry,” she notes.
Chris Bates explains that there are endless possibilities for the chemistry of “A” and “B” blocks. “Modern synthetic chemistry allows us to pick basically any type of A polymer and connect it with a different B block,” he says. “Given this vast design space, the real challenge is figuring out the most crucial knobs to turn that control self-assembly.” Morgan was trying to understand that relationship between chemistry and structure.
She recalls the process that led to the discovery: “I had chemically tweaked a parameter related to what is called ‘conformational asymmetry,’ which describes how the two blocks fill space. We weren’t necessarily trying to find a new phase but thought that maybe we’d uncover some new behavior. In this case, the A and B blocks that are covalently tied together fill space very differently, and that seems to be the underlying parameter that gives rise to some unique self-assembly.”
After creating the block copolymers, she took them to the Advanced Photon Source at Argonne National Laboratory, in Illinois, where a technique called “small-angle X-ray scattering” was used to characterize them. The process yields a two-dimensional signature of scattered X-rays arranged in concentric rings. The relative placement and intensity of the rings indicates a particular phase. Morgan needed to travel to a national lab, because the process requires X-rays more powerful than what can be produced on campus.
After that work, says Chris, “Using knowledge of crystallography, you can interpret the scattering data and produce an image as if you were looking at the structure with your eye. And in this case, the data was of such high quality that we were able to do that unambiguously.”
Morgan recalls that when she examined the X-ray pattern, one thing was unmistakably clear: “It looked different. I thought, ‘What is that?’”
It was, of course, their newly discovered phase, known as A15. “With these types of AB block copolymers, there are only a handful of phases that people have observed previously, and we’ve found another one, which adds to the palette of possible options from a design standpoint,” Chris says.
“Among the ways of categorizing structures, this phase belongs to a class known as ‘tetrahedrally close-packed’,” adds Lequieu, an expert in computer simulations who modeled the phase behavior of polymers. “The phase we’ve found in block copolymers was actually first observed in 1931 with an allotrope [or form] of tungsten. But in that case, A15 forms from metal atoms, which create a very small structure at the atomic length scale. Our block copolymers adopt the same structure but at a length scale two orders of magnitude larger, and, of course, no metal atoms are involved.
“If you were to look at both with a microscope, their structures would look the same, but just at different sizes . It’s fascinating that nature chooses to use the same structural motifs for completely different materials having entirely unrelated chemistry and physics.”
The project demonstrates the ease of, and proclivity for, collaboration among UCSB researchers. It began with new chemistry developed by Hawker and Bates to tune the properties of materials, which was followed by Morgan’s unexpected characterization results. “From there, we went to Josh and told him there’s something strange in the experiments that we didn’t expect and asked him why,” Chris says. Lequieu then worked with Fredrickson to develop the computer simulations.
“There was a really nice back and forth on this project,” Lequieu says. “An experiment was done that was challenging to understand, so we performed simulations to explain it. Morgan then did more experiments, informed by the results of the initial simulations, and observed that the computations were actually predictive. The phases observed experimentally showed up right where the simulations said they would. In some places, however, the experiments and simulations disagreed, so we iterated multiple times to improve the models and really understand the subtleties involved.”
“Moving forward,” Chris adds, “our team continues to integrate materials synthesis and theory in a search of more unique phase behavior.”
Lequieu describes the feedback loop from experiment to simulation to theory and back around as “sort of the dream of modern materials science. It takes a lot of work for Morgan to make these samples. It’s much easier if someone predicts outcomes on a computer and can say, ‘Here’s a subset of polymers to synthesize that should form the desired structure.’ This so-called ‘inverse design’ approach saves her a lot of time and effort.”
In terms of nature falling back on preferred designs for otherwise unrelated materials, a bit of history is worth noting. In 1887, Lord Kelvin — he of the eponymous units of absolute temperature — was working on what later came to be known as the “Kelvin problem.” It was an effort to determine how space could be partitioned into cells of equal volume with the least surface area between them. His proposed solution, which indicated the most efficient bubble foam, became known as the “Kelvin structure.”
It held for about a hundred years, but in 1994 was shown to be incorrect. Kelvin had chosen what could be called “Structure A,” but a team of British scientists showed that “Structure B” was even better. Since then, Structure B has gained fame in scientific circles and even well beyond, appearing, for instance, in the form of giant bubbles that serve as both functional architectural elements and design elements on the roof of the Beijing National Aquatics Center built for the 2008 Olympics.
It turns out that the new phase, A15, discovered by the researchers in this project is Structure B, confirming once again that nature likes a previously successful design.