REPORTS
7. H. V. Borgaonkar, S. R. Raverkar, S. B. Chandalia,
particles have substantially more of them. If these and fresh toluene was added. No metal was ob-
low coordination number corner and/or edge po- served to have leached into the liquid phase
sitions are implicated as active sites for toluene during reaction, and the decanted liquid showed
oxidation, then their relatively higher occur- no further reaction in the absence of catalyst
rence in the Au-Pd/C sample could account for (fig. S7 and table S16). The reaction was then
the superior performance displayed by this cat- allowed to proceed for a further 7 hours, and the
alyst. Another possible explanation could lie in whole process was repeated a further two times.
the difference in the distribution of Au-Pd par- The reaction profile obtained with the decanta-
ticle morphologies found in the two catalyst tion experiments was identical to that obtained
samples. The Au-Pd/C catalyst predominantly with the fresh catalyst (fig. S8). Detailed STEM
has multiply twinned (icosahedral and decahe- characterization shows that there is minimal
dral) particles, which tend to have {111} facet particle growth or morphology change for the
terminations. In comparison, the Au-Pd/TiO2 Au-Pd/C catalysts when studied over an ex-
materials show an increased fraction of cub- tended reaction period (Fig. 1), during which
octahedral and singly/doubly twinned particles, catalysts were recovered after 31 and 65 hours of
which exhibit mixed {100}/{111} facet ter- reaction, followed by two reuse cycles of 7 hours
minations. Hence, the increasing proportion of (figs. S9 and S10). Therefore, it is clear that any
{100}-type facets in the Au-Pd/TiO2 sample cor- sintering or structural modification of these highly
relates with a lowering of the catalytic activity, active catalysts is minimal, and we consider them
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Company through the Dow Methane Challenge.
and preparation strategies need to avoid them.
In a final set of experiments, we investigated
the stability of the catalysts, because it is crucial
to confirm that high-activity catalysts can be re-
used. With the Au-Pd/TiO2 catalyst, the reaction
was stopped after 7 hours, and the catalyst was
recovered by decantation. Identical conversion
was obtained on reuse of the Au-Pd/TiO2 catalyst
(Table 1, entries 14 and 15). For the Au-Pd/C
catalyst, the reaction was stopped after 7 hours
and the catalyst was allowed to settle. The liquid
phase was then carefully removed by decantation
to be stable and reusable.
References and Notes
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Supporting Online Material
Materials and Methods
Figs. S1 to S10
Tables S1 to S16
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References
29 September 2010; accepted 14 December 2010
10.1126/science.1198458
Appl. Catal. A Gen. 273, 143 (2004).
between these fields. Therefore, combining am-
phiphilicity with colloidal rigidity, we study “Janus
spheres” that are hydrophobic on one hemi-
sphere and negatively charged on the other.
An earlier publication from this laboratory de-
scribed some structures that these hybrid ma-
terials form (18). Here, we address the kinetics of
self-assembly at the single-particle level, showing
that small, kinetically favored isomers join to
form highly ordered but nonequilibrium large-
scale structures.
A critical design rule is that the range of
interparticle interactions (hydrophobic attraction
and electrostatic repulsion) must be short relative
to particle size and that the interactions must be
reversible. Clustering then favors densely packed
Supracolloidal Reaction Kinetics of
Janus Spheres
Qian Chen,1 Jonathan K. Whitmer,1,2 Shan Jiang,1 Sung Chul Bae,1 Erik Luijten,3,4* Steve Granick1,2,5
*
Clusters in the form of aggregates of a small number of elemental units display structural,
thermodynamic, and dynamic properties different from those of bulk materials. We studied the kinetic
pathways of self-assembly of “Janus spheres” with hemispherical hydrophobic attraction and found key
differences from those characteristic of molecular amphiphiles. Experimental visualization combined
with theory and molecular dynamics simulation shows that small, kinetically favored isomers fuse,
before they equilibrate, into fibrillar triple helices with at most six nearest neighbors per particle. The time
scales of colloidal rearrangement combined with the directional interactions resulting from Janus geometry
make this a prototypical system to elucidate, on a mechanistic level and with single-particle kinetic
resolution, how chemical anisotropy and reaction kinetics coordinate to generate highly ordered structures.
lusters, an intermediate level of matter structures that result from isotropic interactions be- structures with at most six nearest neighbors per
between building block (atom, molecule, tween building blocks are well understood (5–8), particle, in contrast to the more open and less
or particle) and bulk phase, are found ubiq- it is more challenging to understand clusters formed ordered structures formed by particles whose in-
C
uitously in nature and technology—for example, from the common case of directional noncovalent teraction range is larger (13). At very low salt
in the nucleation of bulk phases (1), nanoparticles interactions (9–17). On this question, we note that concentrations, particles repel one another electro-
(2), and protein aggregates in biology (3,4). Whereas for molecular amphiphiles, such as surfactants, statically, whereas at high salt concentrations, van
phospholipids, and many block copolymers, the der Waals forces cause the particles to aggregate
segregation of their polar and nonpolar portions irreversibly (19). Therefore, we consider interme-
is a major mechanism steering the spontaneous diate concentrations of monovalent salt at which
formation of microstructured mesophases with amphiphilic clusters self-assemble (20).
1Department of Materials Science and Engineering, University
of Illinois, Urbana, IL 61801, USA. 2Department of Physics,
University of Illinois, Urbana, IL 61801, USA. 3Department of
Materials Science and Engineering, Northwestern University,
Evanston, IL 60208, USA. 4Department of Engineering Sciences
and Applied Mathematics, Northwestern University, Evanston,
IL 60208, USA. 5Department of Chemistry, University of Illinois,
Urbana, IL 61801, USA.
fascinating and useful structures (9–11). Sim-
If the hydrophobic patch is too small, as-
ilarly, colloidal particles, larger than molecules sembly admits clusters composed of at most four
but small enough to sustain Brownian motion, particles. However, increase in patch size allows
also assemble into clusters owing to directional such clusters to grow into larger assemblies, with
noncovalent interactions (12–17). A largely un- two constraints: First, particles must approach
solved problem is the question of commonality closely enough to experience hydrophobic attrac-
*To whom correspondence should be addressed. E-mail:
luijten@northwestern.edu (E.L.); sgranick@illinois.edu (S.G.)
199