2,854 research outputs found

    Development of reclaimed potable water quality criteria

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    In order to minimize launch requirements necessary to meet the demands of long-term spaceflight, NASA will reuse water reclaimed from various on-board sources including urine, feces, wash water and humidity condensate. Development of reclamation systems requires the promulgation of water quality standards for potable reuse of the reclaimed water. Existing standards for domestic U.S. potable water consumption were developed, but do not consider the peculiar problems associated with the potable reuse of recycled water. An effort was made to: (1) define a protocol by which comprehensive reclaimed water potability/palatability criteria can be established and updated; and (2) continue the effort to characterize the organic content of reclaimed water in the Regenerative Life Support Evaluation

    Absorption/Expulsion of Oligomers and Linear Macromolecules in a Polymer Brush

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    The absorption of free linear chains in a polymer brush was studied with respect to chain size LL and compatibility χ\chi with the brush by means of Monte Carlo (MC) simulations and Density Functional Theory (DFT) / Self-Consistent Field Theory (SCFT) at both moderate, σg=0.25\sigma_g = 0.25, and high, σg=1.00\sigma_g = 1.00, grafting densities using a bead-spring model. Different concentrations of the free chains 0.0625ϕo0.3750.0625 \le \phi_o \le 0.375 are examined. Contrary to the case of χ=0\chi = 0 when all species are almost completely ejected by the polymer brush irrespective of their length LL, for χ<0\chi < 0 we find that the degree of absorption (absorbed amount) Γ(L)\Gamma(L) undergoes a sharp crossover from weak to strong (100\approx 100%) absorption, discriminating between oligomers, 1L81\le L\le 8, and longer chains. For a moderately dense brush, σg=0.25\sigma_g = 0.25, the longer species, L>8L > 8, populate predominantly the deep inner part of the brush whereas in a dense brush σg=1.00\sigma_g = 1.00 they penetrate into the "fluffy" tail of the dense brush only. Gyration radius RgR_g and end-to-end distance ReR_e of absorbed chains thereby scale with length LL as free polymers in the bulk. Using both MC and DFT/SCFT methods for brushes of different chain length 32N25632 \le N \le 256, we demonstrate the existence of unique {\em critical} value of compatibility χ=χc<0\chi = \chi^{c}<0. For χc(ϕo)\chi^{c}(\phi_o) the energy of free chains attains the {\em same} value, irrespective of length LL whereas the entropy of free chain displays a pronounced minimum. At χc\chi^{c} all density profiles of absorbing chains with different LL intersect at the same distance from the grafting plane. The penetration/expulsion kinetics of free chains into the polymer brush after an instantaneous change in their compatibility χ\chi displays a rather rich behavior. We find three distinct regimes of penetration kinetics of free chains regarding the length LL: I (1L81\le L\le 8), II (8LN8 \le L \le N), and III (L>NL > N), in which the time of absorption τ\tau grows with LL at a different rate. During the initial stages of penetration into the brush one observes a power-law increase of Γtα\Gamma \propto t^\alpha with power αlnϕo\alpha \propto -\ln \phi_o whereby penetration of the free chains into the brush gets {\em slower} as their concentration rises

    Universal Formulae for Percolation Thresholds

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    A power law is postulated for both site and bond percolation thresholds. The formula writes pc=p0[(d1)(q1)]ad bp_c=p_0[(d-1)(q-1)]^{-a}d^{\ b}, where dd is the space dimension and qq the coordination number. All thresholds up to dd\rightarrow \infty are found to belong to only three universality classes. For first two classes b=0b=0 for site dilution while b=ab=a for bond dilution. The last one associated to high dimensions is characterized by b=2a1b=2a-1 for both sites and bonds. Classes are defined by a set of value for {p0; a}\{p_0; \ a\}. Deviations from available numerical estimates at d7d \leq 7 are within ±0.008\pm 0.008 and ±0.0004\pm 0.0004 for high dimensional hypercubic expansions at d8d \geq 8. The formula is found to be also valid for Ising critical temperatures.Comment: 11 pages, latex, 3 figures not include

    Entropy-driven phase transition in a system of long rods on a square lattice

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    The isotropic-nematic (I-N) phase transition in a system of long straight rigid rods of length k on square lattices is studied by combining Monte Carlo simulations and theoretical analysis. The process is analyzed by comparing the configurational entropy of the system with the corresponding to a fully aligned system, whose calculation reduces to the 1D case. The results obtained (1) allow to estimate the minimum value of k which leads to the formation of a nematic phase and provide an interesting interpretation of this critical value; (2) provide numerical evidence on the existence of a second phase transition (from a nematic to a non-nematic state) occurring at density close to 1 and (3) allow to test the predictions of the main theoretical models developed to treat the polymers adsorption problem.Comment: 14 pages, 6 figures. Accepted for publication in JSTA

    Isotopic carbon analysis of meteoritic organic matter

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    Isotopic carbon analysis of meteoritic organic matte

    Topological analysis of polymeric melts: Chain length effects and fast-converging estimators for entanglement length

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    Primitive path analyses of entanglements are performed over a wide range of chain lengths for both bead spring and atomistic polyethylene polymer melts. Estimators for the entanglement length N_e which operate on results for a single chain length N are shown to produce systematic O(1/N) errors. The mathematical roots of these errors are identified as (a) treating chain ends as entanglements and (b) neglecting non-Gaussian corrections to chain and primitive path dimensions. The prefactors for the O(1/N) errors may be large; in general their magnitude depends both on the polymer model and the method used to obtain primitive paths. We propose, derive and test new estimators which eliminate these systematic errors using information obtainable from the variation of entanglement characteristics with chain length. The new estimators produce accurate results for N_e from marginally entangled systems. Formulas based on direct enumeration of entanglements appear to converge faster and are simpler to apply.Comment: Major revisions. Developed near-ideal estimators which operate on multiple chain lengths. Now test these on two very different model polymers

    Polymer Brushes in Cylindrical Pores: Simulation versus Scaling Theory

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    The structure of flexible polymers endgrafted in cylindrical pores of diameter D is studied as a function of chain length N and grafting density \sigma, assuming good solvent conditions. A phenomenological scaling theory, describing the variation of the linear dimensions of the chains with \sigma, is developed and tested by Molecular Dynamics simulations of a bead-spring model.Comment: 35 pages, 38 figure

    Sub-millimeter Spectroscopy of Astrophysically Important Molecules and Ions: Metal Hydrides, Halides, and Cyanides

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    With the advent of SOFIA, Herschel, and SAFIR, new wavelength regions will become routinely accessible for astronomical spectroscopy, particularly at submm frequencies (0.5-1.1 THz). Molecular emission dominates the spectra of dense interstellar gas at these wavelengths. Because heterodyne detectors are major instruments of these missions, accurate knowledge of transition frequencies is crucial for their success. The Ziurys spectroscopy laboratory has been focusing on the measurement of the pure rotational transitions of astrophysically important molecules in the sub-mm regime. Of particular interest have been metal hydride species and their ions, as well as metal halides and cyanides. A new avenue of study has included metal bearing molecular ions

    Static and dynamic heterogeneities in a model for irreversible gelation

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    We study the structure and the dynamics in the formation of irreversible gels by means of molecular dynamics simulation of a model system where the gelation transition is due to the random percolation of permanent bonds between neighboring particles. We analyze the heterogeneities of the dynamics in terms of the fluctuations of the intermediate scattering functions: In the sol phase close to the percolation threshold, we find that this dynamical susceptibility increases with the time until it reaches a plateau. At the gelation threshold this plateau scales as a function of the wave vector kk as kη2k^{\eta -2}, with η\eta being related to the decay of the percolation pair connectedness function. At the lowest wave vector, approaching the gelation threshold it diverges with the same exponent γ\gamma as the mean cluster size. These findings suggest an alternative way of measuring critical exponents in a system undergoing chemical gelation.Comment: 4 pages, 4 figure

    Local and chain dynamics in miscible polymer blends: A Monte Carlo simulation study

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    Local chain structure and local environment play an important role in the dynamics of polymer chains in miscible blends. In general, the friction coefficients that describe the segmental dynamics of the two components in a blend differ from each other and from those of the pure melts. In this work, we investigate polymer blend dynamics with Monte Carlo simulations of a generalized bond-fluctuation model, where differences in the interaction energies between non-bonded nearest neighbors distinguish the two components of a blend. Simulations employing only local moves and respecting a non-bond crossing condition were carried out for blends with a range of compositions, densities, and chain lengths. The blends investigated here have long-chain dynamics in the crossover region between Rouse and entangled behavior. In order to investigate the scaling of the self-diffusion coefficients, characteristic chain lengths NcN_\mathrm{c} are calculated from the packing length of the chains. These are combined with a local mobility μ\mu determined from the acceptance rate and the effective bond length to yield characteristic self-diffusion coefficients Dc=μ/NcD_\mathrm{c}=\mu/N_\mathrm{c}. We find that the data for both melts and blends collapse onto a common line in a graph of reduced diffusion coefficients D/DcD/D_\mathrm{c} as a function of reduced chain length N/NcN/N_\mathrm{c}. The composition dependence of dynamic properties is investigated in detail for melts and blends with chains of length twenty at three different densities. For these blends, we calculate friction coefficients from the local mobilities and consider their composition and pressure dependence. The friction coefficients determined in this way show many of the characteristics observed in experiments on miscible blends.Comment: 12 pages, 13 figures, editorial change
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