53 research outputs found

    Microbubbles and Cavitation

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    The present report arose from a joint effort of the California Institute of Technology, The Catholic University of America and the David Taylor Naval Ship Research and Development Center. The initial purpose was to document by both light-scattering and holographic techniques the distribution of microbubbles in laboratory cavitation test facilities (under different conditions of cavitation testing), to compare these two different techniques where feasible and then, as the last stage, to make similar observations of nuclei in natural or oceanic waters. It has been apparent to many workers in the field of cavitation inception that there has not yet been adequate correlation of laboratory and field conditions for cavitation testing - particularly for cavitation inception testing. Thus the proposed work offered the first real opportunity to explore this important connection. Caltech's role in this work was to design and build a holographic system that would be suitable for use either in the laboratory or the field. In the first case we anticipated making laboratory nuclei observations in the Institute's Low Turbulence Water Tunnel (LTWT) jointly with the light-scattering device designed by Professor S. C. Ling of C.U.A. and developed further by Mr. S. Gowing of DTNSRDC. For the latter case, the field work, it was proposed to install the holographic system in a submersible tank to permit holographic recordings of a suitable test volume of fluid. As an initial goal a depth of 100 feet was selected for the maximum depth of operation

    Sliding Phases in XY-Models, Crystals, and Cationic Lipid-DNA Complexes

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    We predict the existence of a totally new class of phases in weakly coupled, three-dimensional stacks of two-dimensional (2D) XY-models. These ``sliding phases'' behave essentially like decoupled, independent 2D XY-models with precisely zero free energy cost associated with rotating spins in one layer relative to those in neighboring layers. As a result, the two-point spin correlation function decays algebraically with in-plane separation. Our results, which contradict past studies because we include higher-gradient couplings between layers, also apply to crystals and may explain recently observed behavior in cationic lipid-DNA complexes.Comment: 4 pages of double column text in REVTEX format and 1 postscript figur

    Sliding Columnar Phase of DNA-Lipid Complexes

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    We introduce a simple model for DNA-cationic-lipid complexes in which galleries between planar bilayer lipid lamellae contain DNA 2D smectic lattices that couple orientationally and positionally to lattices in neighboring galleries. We identify a new equilibrium phase in which there are long-range orientational but not positional correlations between DNA lattices. We discuss properties of this new phase such as its X-ray structure factor S(r), which exhibits unusual exp(- const.ln^2 r) behavior as a function of in-plane separation r.Comment: This file contains 4 pages of double column text and one postscript figure. This version includes interactions between dislocations in a given gallery and presents an improved estimate of the decoupling temperature. It is the published versio

    Random Packings of Frictionless Particles

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    We study random packings of frictionless particles at T=0. The packing fraction where the pressure becomes nonzero is the same as the jamming threshold, where the static shear modulus becomes nonzero. The distribution of threshold packing fractions narrows and its peak approaches random close-packing as the system size increases. For packing fractions within the peak, there is no self-averaging, leading to exponential decay of the interparticle force distribution.Comment: 4 pages, 3 figure

    Force distributions near the jamming and glass transitions

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    We calculate the distribution of interparticle normal forces P(F)P(F) near the glass and jamming transitions in model supercooled liquids and foams, respectively. P(F)P(F) develops a peak that appears near the glass or jamming transitions, whose height increases with decreasing temperature, decreasing shear stress and increasing packing density. A similar shape of P(F)P(F) was observed in experiments on static granular packings. We propose that the appearance of this peak signals the development of a yield stress. The sensitivity of the peak to temperature, shear stress and density lends credence to the recently proposed generalized jamming phase diagram.Comment: 4 pages, 3 postscript figures;Version 3 replaces figure 1 and removes figure 2 from version 1. Significant rewording of version 1 to emphasize the formation of peak in P(F) when these systems jam along five different routes of the recently proposed jamming phase diagram. Version 2 displayed the incorrect abstrac

    Lyapunov spectral analysis of a nonequilibrium Ising-like transition

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    By simulating a nonequilibrium coupled map lattice that undergoes an Ising-like phase transition, we show that the Lyapunov spectrum and related dynamical quantities such as the dimension correlation length~ξδ\xi_\delta are insensitive to the onset of long-range ferromagnetic order. As a function of lattice coupling constant~gg and for certain lattice maps, the Lyapunov dimension density and other dynamical order parameters go through a minimum. The occurrence of this minimum as a function of~gg depends on the number of nearest neighbors of a lattice point but not on the lattice symmetry, on the lattice dimensionality or on the position of the Ising-like transition. In one-space dimension, the spatial correlation length associated with magnitude fluctuations and the length~ξδ\xi_\delta are approximately equal, with both varying linearly with the radius of the lattice coupling.Comment: 29 pages of text plus 15 figures, uses REVTeX macros. Submitted to Phys. Rev. E
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