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Scientific and Technical Aerospace Reports Volume 39 April 6, 2001

Scientific and Technical Aerospace Reports Volume 39 April 6, 2001

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cal transducers. Additionally, the ability to experimentally probe colloidal suspensions interacting through tunable anisotropic<br />

potentials is of fundamental interest. In this talk we will describe our work toward a microscopic underst<strong>and</strong>ing of magnetorheological<br />

behavior. Much of the rheological behavior arises from the cross-linked structure caused by defects <strong>and</strong> L<strong>and</strong>au-Peierls<br />

thermal fluctuations of dipolar chains. We used the light scattering technique, diffusing-wave spectroscopy, to investigate the fluctuations<br />

of dipolar chains. We have prepared monodisperse neutrally buoyant MR suspensions allowing us to probe the dynamics<br />

of the dipolar chains using light scattering without complications due to gravitational forces <strong>and</strong> polydispersity. Optical gradient<br />

force trapping techniques, or laser tweezers, have become increasingly important tools for studying the microscopic structure,<br />

mechanics, <strong>and</strong> interactions in biological, colloidal, <strong>and</strong> macromolecular materials. We also present our study of the micromechanical<br />

properties of dipolar chains <strong>and</strong> chain aggregates in a magnetorheological suspension. Using dual-trap optical tweezers,<br />

we are able to directly measure the deformation of dipolar chains parallel <strong>and</strong> perpendicular to the applied magnetic field. We<br />

observe the field-dependence of chain mechanical properties, such as tensile strain, chain reorganization, defect-annealing <strong>and</strong><br />

rupture. We discuss the role these forms of energy dissipation take in the yield stress <strong>and</strong> rheology of MR suspensions.<br />

Author (revised)<br />

Magnetorheological Fluids; Suspensions; Crosslinking; Colloids<br />

<strong>2001</strong>0024902 Colorado Univ., Dept. of Physics, Boulder, CO USA<br />

Freely Suspended Smectic Filaments <strong>and</strong> the Structure of the B7 Phase of MHOBOW<br />

Clark, N., Colorado Univ., USA; Link, D. R., Colorado Univ., USA; Maclennan, J. E., Colorado Univ., USA; Proceedings of the<br />

Fifth Microgravity Fluid Physics <strong>and</strong> Transport Phenomena Conference; December 2000, pp. 337-3<strong>39</strong>; In English; See also<br />

<strong>2001</strong>0024890; No Copyright; Abstract Only; Available from CASI only as part of the entire parent document<br />

Our recent discovery of the spontaneous formation of chiral domains in fluid smectic phases of achiral bow-shaped molecules<br />

opens up a wide variety of possibilities for new liquid crystal phases <strong>and</strong> phenomena. The basic, spontaneously chiral layer structure<br />

of the highest temperature fluid smectic phases, the B2 <strong>and</strong> B7, are shown. One of the most intriguing aspects of this structure<br />

is the plethora of possible phases coming from different stacking sequences of the polar ordering <strong>and</strong> tilt directions. The four possibilities<br />

of next-nearest neighbor alternation are shown. In the original material studied, NOBOW, the ground states found are antiferroelectric,<br />

either the racemic SmC(sub S)P(sub A) or the chiral SmC(sub A)P(sub A). We are currently studying MHOBOW,<br />

synthesized by D. Walba which, by virtue of its methyl hexyloxy tail has a tendency to form anticlinic layer interfaces, in the hope<br />

of finding a phase with a ferroelectric ground state, either SmC(sub A)P(sub S) or SmC(sub S)P(sub A), which can be obtained<br />

in NOBOW only by applying a field. Preliminary observations of MHO-BOW have made its study, from the point of view of<br />

underst<strong>and</strong>ing novel LC structures, extremely high priority. The following truly remarkable characteristics have been revealed:<br />

(i) The smectic phase grows out of the isotropic in the form of helical ribbons. The resulting planar aligned textures of focal conics<br />

with layers normal to glass plates exhibit bizarre modulations, including stripes <strong>and</strong> checker-boards. These have also been seen<br />

in other materials suggesting that this is a new phase (tentatively called B7), which is a fluid smectic with some kind of in-layer<br />

structure. (ii) It is virtually impossible to make freely suspended films of MHOBOW. Rather it makes the freely suspended filaments<br />

which preliminary x-ray scattering experiments reveal to have the nested cylinder layer structure indicated; (iii) The powder<br />

x-ray diffraction exhibits four resolution-limited smectic layering peaks, very close in layer spacing, which vary continuously with<br />

T. This is further evidence for a more complex three dimensional structure than NOBOW, which has a typical single layering<br />

reflection. (iv) The x-ray structure factor of the layering peak of the filaments is extraordinarily complex <strong>and</strong> rich. Varying in qL<br />

(the scattering vector component along the filament axis) from a double slit-like pattern to modulated layer-like patterns, as qH<br />

(the scattering vector component normal to the filament axis) is varied over the range where the four powder peaks are located.<br />

These results suggest some kind of mosaic structure, perhaps with different layer spacings corresponding to the different stacking<br />

sequences. Recent x-ray diffraction experiments show that the peaks are modulated in intensity upon translation along a filament,<br />

in domains of several hundred microns dimension. These preliminary experiments suggest that the B7 is a fluid smectic with<br />

extremely unusual <strong>and</strong> fascinating structures. of all of the many hundreds of fluid smectic materials we have attempted to study<br />

in the freely suspended film geometry over the years, only a few have failed to form films, <strong>and</strong> none showed any great tendency<br />

to form filaments, although this clearly should be a possible freely suspended smectic LC morphology. On several ocCASIons<br />

in the past we have intentionally tried to make filaments from a variety of smectics without success. Thus the smectic filament<br />

formation property makes the B7 phase unique. It seems quite likely that the stability of filaments is related to the in-plane structure.<br />

The filaments exhibit other interesting structural <strong>and</strong> optical features. They are birefringent with a local optic axis which is<br />

oblique <strong>and</strong> which can vary continuously along filament <strong>and</strong> which can be manipulated with an electric field applied normal to<br />

the fiber, as if the field were causing a rotation of the optic axis about the fiber axis. Rapid displacement of the ends of the fiber<br />

71

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