2012
DOI: 10.1039/c1sm06794j
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The mobilities of micro- and nano-particles at interfaces of nematic liquid crystals

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Cited by 18 publications
(25 citation statements)
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“…Nematic LCs possess direction-dependent (Miesowicz) shear viscosities with the direction of lowest viscosity being parallel to the director. 2931 In common thermotropic liquid crystals, the Miesowicz viscosity corresponding to shear flow with velocity perpendicular to the director is often ~10× larger than the viscosity parallel to the director. 29 Because experimental determination of Miesowicz viscosities of lyotropic LCs is difficult as general and facile methods to manipulate the surface anchoring of lyotropic LC phases do not exist, we estimated the apparent viscosity experienced by the motile P. mirabilis-flhDC in nematic DSCG to be μ~ 0.7 Pa·s by comparing the average velocity in nematic DSCG to previous measurements of P. mirabilis-flhDC motility in solutions of known viscosity.…”
Section: Resultsmentioning
confidence: 99%
“…Nematic LCs possess direction-dependent (Miesowicz) shear viscosities with the direction of lowest viscosity being parallel to the director. 2931 In common thermotropic liquid crystals, the Miesowicz viscosity corresponding to shear flow with velocity perpendicular to the director is often ~10× larger than the viscosity parallel to the director. 29 Because experimental determination of Miesowicz viscosities of lyotropic LCs is difficult as general and facile methods to manipulate the surface anchoring of lyotropic LC phases do not exist, we estimated the apparent viscosity experienced by the motile P. mirabilis-flhDC in nematic DSCG to be μ~ 0.7 Pa·s by comparing the average velocity in nematic DSCG to previous measurements of P. mirabilis-flhDC motility in solutions of known viscosity.…”
Section: Resultsmentioning
confidence: 99%
“…Our experimental results reported above and recent coarse grain modelling [25] support, however, the proposition that elastic distortions (and defect core energies) are minimized by the partitioning of a colloid to a defect. Accordingly, we estimate the magnitude of the elastic forces driving the colloid to the defect as: [34, 35] …”
Section: Resultsmentioning
confidence: 99%
“…Our experimental results reported above and recent coarse grain modelling [ 25 ] support, however, the proposition that elastic distortions (and defect core energies) are minimized by the partitioning of a colloid to a defect. Accordingly, we estimate the magnitude of the elastic forces driving the colloid to the defect as: [ 34,35 ] = E Ka elastic (1) in which K is the elastic constant of the LC (using the "one constant" approximation), and a is the radius of the PS colloid (0.5 µm). Using a typical value for an elastic constant for a low molecular weight LC, K = 10 −11 N, [ 20,36 ] we calculate E elastic ≈ 5 × 10 −18 J.…”
Section: Resultsmentioning
confidence: 99%
“…The dark-field microscopy allows direct real-time visualization of colloidal particles smaller than the diffraction limit [21,[26][27][28]30,32,45] due to the strong scattering of visible light from gold NPs [50] having the appearance of bright spots on a dark, uniform background. The size of these spots does not directly correspond to the actual dimensions of the NPs but represents their scattering cross section that, in addition to the particle size, is determined by diffraction-limited resolution [50].…”
Section: A Diffusion Of Rodlike Convex Pentagonal Nanoprisms Alignedmentioning
confidence: 99%
“…It was found that the diffusivity of gold NPs can be affected by chemical functionalization of their surface [25] and the mobility of gold NPs on the LC-aqueous interface is significantly different relative to microparticles insensitive to the details of the interfacial environment [32].…”
Section: Introductionmentioning
confidence: 99%