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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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aries are observed to move if the vibration amplitude is large enough. Here, the lower boundary of the film is in contact with the<br />

bulk suspension, <strong>and</strong> the mechanical vibration is coupled to the film through capillary waves excited on the bulk surface due to<br />

the Faraday instability. A series of pictures in a figure show how typically grain boundaries evolve under vibration with a frequency<br />

of about 100 Hz. The total length of the grain boundaries decreases, usually in a monotonic fashion, <strong>and</strong> finally disappears.<br />

The detail process of grain boundary migration is in general rather complex, because the mobility of a grain boundary depends<br />

not only on the relative orientation of the two grains, but also on the direction of the boundary. As a result the mobility is not a<br />

constant but varies along the boundary. However, the evolution of grain boundaries under external forcing does show certain simple<br />

features: (1) Small loops of defect lines are eliminated first, as seen in a figure, <strong>and</strong> the effect is somewhat similarly to domain<br />

coarsening seen in phase-separating fluids. (2) Before the merging of two domains, the boundary between them becomes fuzzy<br />

<strong>and</strong> discontinuous. Observations under the high power magnification show a rather continuous transition from the large- to the<br />

small-angle grain boundaries. In the process, domains are seen to rotate coherently. (3) The elimination of small-angle grain<br />

boundaries is much more rapid than the large-angle ones. The application of the external vibration not only offers a mean of studying<br />

defect dynamics but also provides a robust way to grow high-quality 2D single colloidal crystals of size never achieved before.<br />

Because the assembly process relies on the capillary force, particles of different materials <strong>and</strong> with various surface properties can<br />

be crystallized in this way. Since the freely suspended film provides an environment similar to biological membranes, the technique<br />

may be potentially useful for growing 2D crystals of membrane proteins, of which only a h<strong>and</strong>ful have been successfully<br />

crystallized.<br />

Author (revised)<br />

Colloids; Crystallization; Defects; Grain Boundaries; Migration<br />

<strong>2001</strong>0024952 Harvard Univ., USA<br />

Photonic Crystals Based on Self-Assembly of Colloidal Particles<br />

Weitz, D., Harvard Univ., USA; Proceedings of the Fifth Microgravity Fluid Physics <strong>and</strong> Transport Phenomena Conference; December<br />

2000, pp. 1183-1189; In English; See also <strong>2001</strong>0024890; No Copyright; Avail: CASI; A02, Hardcopy; A10, Microfiche<br />

Photonic crystals are systems in which the refractive index periodically changes in space. These structures show interesting<br />

optical properties which may lead to the suppression of propagation of light within a certain frequency range. During the last years<br />

there have been strong efforts to fabricate such materials with spatial periodicities lying in range of the wavelength of visible light.<br />

One possible approach to fabricate these materials is the use of colloidal particles. We use self-organization of colloidal particles<br />

to produce these periodic structures. by using organic <strong>and</strong> inorganic materials we control both the elastic <strong>and</strong> scattering properties<br />

of the particles <strong>and</strong> the lattice. We determine the structures <strong>and</strong> optical properties of the colloidal crystal by optical microscopy<br />

<strong>and</strong> light scattering experiments. by performing light scattering measurements in the optical microscope simultaneously with<br />

imaging, we study the scattering from a region with known defect structure. These new materials have great potential for a variety<br />

of optical communication devices. Possible technical applications are discussed.<br />

Author (revised)<br />

Colloids; Optical Properties; Scattering; Crystals; Photonics<br />

<strong>2001</strong>0024953 NASA Glenn Research Center, Clevel<strong>and</strong>, OH USA<br />

Gravitational Effects on Flow Instability <strong>and</strong> Transition in Low Density Jets<br />

Agrawal A. K., Oklahoma Univ., USA; Parthasarathy, K., Oklahoma Univ., USA; Pasumarthi, K., Oklahoma Univ., USA; Griffin,<br />

D. W., NASA Glenn Research Center, USA; Proceedings of the Fifth Microgravity Fluid Physics <strong>and</strong> Transport Phenomena Conference;<br />

December 2000, pp. 1190-1192; In English; See also <strong>2001</strong>0024890; No Copyright; Abstract Only; Available from CASI<br />

only as part of the entire parent document<br />

Recent experiments have shown that low-density gas jets injected into a high-density ambient gas undergo an instability<br />

mode, leading to highly-periodic oscillations in the flow-field for certain conditions. The transition from laminar to turbulent flow<br />

in these jets is abrupt, without the gradual change in scales. Even the fine scale turbulent structure repeats itself with extreme regularity<br />

from cycle to cycle. Similar observations were obtained in buoyancy-dominated <strong>and</strong> momentum-dominated jets characterized<br />

by the Richardson numbers, Ri = [gD(rho(sub a)-rho(sub j))/rho(sub j)U(sub j)(exp 2) ] where g is the gravitational<br />

acceleration, D is the jet diameter, rho(sub a) <strong>and</strong> rho(sub a) are, respectively, the free-stream <strong>and</strong> jet densities, <strong>and</strong> U(sub j) is<br />

the mean jet exit velocity. At high Richardson numbers, the instability is presumably caused by buoyancy since the flow-oscillation<br />

frequency (f) or the Strouhal number, St = [fD/U(sub j)] scales with Ri. In momentum-dominated jets, however, the Strouhal<br />

number of the oscillating flow is relatively independent of the Ri. In this case, a local absolute instability is predicted in the potential<br />

core of low-density jets with S [= rho(sub j)/rho(sub a)] is less than 0.7, which agrees qualitatively with experiments. Although<br />

the instability in gas jets of high Richardson numbers is attributed to buoyancy, direct physical evidence has not been acquired<br />

in experiments. If the instability is indeed caused by buoyancy, the near-field flow structure of the jet will change significantly<br />

100

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