Download Spherical confinement of chiral cellulose nanowhiskers

Survey
yes no Was this document useful for you?
   Thank you for your participation!

* Your assessment is very important for improving the workof artificial intelligence, which forms the content of this project

Document related concepts

State of matter wikipedia , lookup

Transcript
Spherical confinement of chiral cellulose nanowhiskers
Supervisors: Jasper Landman, Andrei Petoukhov & Willem Kegel
May 20, 2014
Cellulose nanowhiskers (cellulose nanocrystals, CNCs) are very promising building blocks for sustainable materials in a
wide number of applications[1]. Apart from their mechanical properties, such as a very high strength, CNCs can form a socalled chiral nematic phase at sufficient concentration[2], although the mechanism of chirality transfer from the molecular
scale to the colloidal scale is not yet fully resolved.
It is interesting to see how robust the phase behaviour of CNCs under spherical confinement. We would like to study CNCs
inside spherical (double layer) vesicles and see the phase behaviour that arises as the vesicle dimensions become smaller.
Moreover, the cellulose inside the vesicles may simultaneously influence the shape of the vesicle
Furthermore we would like to solidify the resulting coassemblies to see what optical properties they might have. Not only
would they make very interesting micron-sized ‘lenses’, these cellulose spheres may be ideal candidates for 3D spherical
lasers, something hitherto only observed in droplets of molecular cholesteric liquid crystals in the liquid phase[3].
We will use a number of in-house techniques such as polarisation and confocal optical microscopy to examine the behaviour
of the system at different length scales. In addition, we will use state-of-the-art X-ray scattering and microscopy to study the
local structure of nanoparticles inside the droplets. For this we will use the experimental facilities at the ESRF in Grenoble.
References
[1] S. J. Eichhorn, “Cellulose nanowhiskers: promising materials for advanced applications,” Soft Matter, vol. 7, no. 2, p. 303,
2011.
[2] J.-F. Revol, H. Bradford, J. Giasson, R. H. Marchessault, and D. G. Gray, “Helicoidal self-ordering of cellulose microfibrils in aqueous suspension,” Int. J. Biol. Macromol., vol. 14, pp. 170–172, June 1992.
[3] M. Humar and I. Muševič, “3D microlasers from self-assembled cholesteric liquid-crystal microdroplets,” Optics Express, vol. 18, no. 26, pp. 111–113, 2010.
[4] S. Vignolini, P. J. Rudall, A. V. Rowland, A. Reed, E. Moyroud, R. B. Faden, J. J. Baumberg, B. J. Glover, and U. Steiner,
“Pointillist structural color in Pollia fruit,” Proceedings of the National Academy of Sciences of the United States of America, vol. 109, no. 39, pp. 15712–15, 2012.
(a) (a,b) A chiral nematic film selectively reflects light of the same circular
polarisation as the helicity in the sample. This property is also found in
nature, e.g. in the fruits of Pollia condensata[4] (c,d)
(b) SEM image of an obliquely cut CNC film, which shows the left-handed
helicity into which the individual particles assembled
Figure 1 A dried chiral nematic film of CNCs
1
Contact information
Jasper Landman
H.R. Kruytgebouw, room N709
+31 30 253 3981
[email protected]
Andrei Petoukhov
H.R. Kruytgebouw, room N703
+31 30 253 1167
[email protected]
Student coordinator: Roel Baars
[email protected]
2
Willem Kegel
H.R. Kruytgebouw, room N711
+31 30 253 2873
[email protected]