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  • Cambridge University Press  (2)
  • American Institute of Physics (AIP)  (1)
  • 2000-2004  (3)
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  • 1
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Physics of Fluids 14 (2002), S. 2376-2387 
    ISSN: 1089-7666
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Based on a closed surface of triangles fitted to atomic coordinates determined crystallographically, Brune and Kim [Proc. Natl. Acad. Sci. USA 90, 3835–3839 (1993)] proposed a boundary-element Stokes-flow technique for ab initio computation of a translational diffusion coefficient and the rotational diffusion tensor Dr of globular proteins. They applied their approach to atomic coordinates for a tetragonal structure of hen egg-white lysozyme, and reported that computed values of a translational diffusion coefficient and Dr=tr(Dr)/3 agreed well with experiment. After establishing the identity between the infinite-dilution tracer diffusion coefficient of the protein macroion (D+ for lysozyme cation) and the "translational diffusion coefficient" computed by Brune and Kim, we adopt a somewhat different computational approach and show how convergence of D+ and Dr for tetragonal lysozyme depends on two computational parameters characterizing the fidelity of the geometric approximation to the protein surface and two others characterizing the accuracy of the Stokes-flow computations. We then compute D+ and Dr for lysozyme using atomic coordinates for the triclinic crystal structure, three structures determined by nuclear magnetic resonance spectroscopy in the liquid phase (presumably corresponding more closely to in vivo structures), the solvated tetragonal structure (with 108 water molecules) considered by Brune and Kim, and a "dry" version of the same structure. These computations show that D+ and Dr computed for all of the dry crystal structures are in excellent agreement with those for the liquid-phase conformations. Values of D+ and Dr computed for the solvated structure are lower, consistent with the larger volume and area of the corresponding polyhedral surface. We also show that several choices of the origin of the force system [discussed by Brenner, J. Colloid Interface Sci. 23, 407–436 (1967)] give rise to nearly identical translational diffusion coefficients. Finally, we show how to estimate the thickness of the "solvation shell" contributing to the hydrodynamic resistance of the protein cation, and use the binary Nernst–Hartley equation to then estimate the effective cation charge at the two pH values at which the binary diffusion coefficient has been accurately measured in recent interferometric experiments. © 2002 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 2
    Publication Date: 2004-06-25
    Description: For spiral Poiseuille flow with radius ratios η ≡ Ri/Ro = 0.77 and 0.95, we have computed complete linear stability boundaries, where Ri and Ro are the inner and outer cylinder radii, respectively. The analysis accounts for arbitrary disturbances of infinitesimal amplitude over the entire range of Reynolds numbers Re for which the flow is stable for some range of Taylor number Ta, and extends previous work to several non-zero rotation rate ratios μ ≡ Ωo/Ωi, where Ωi and Ωo are the (signed) angular speeds. For each combination of μ and η, there is a wide range of Re for which the critical Ta is nearly independent of Re, followed by a precipitous drop to Ta = 0 at the Re at which non-rotating annular Poiseuille flow becomes unstable with respect to a Tollmien-Schlichting-like disturbance. Comparison is also made to a wealth of experimental data for the onset of instability. For Re 〉 0, we compute critical values of Ta for most of the μ = 0 data, and for all of the non-zero-μ data. For μ = 0 and η = 0.955, agreement with data from an annulus with aspect ratio (length divided by gap) greater than 570 is within 3.2% for Re ≤ 325 (based on the gap and mean axial speed), strongly suggesting that no finite-amplitude instability occurs over this range of Re. At higher Re, onset is delayed, with experimental values of Tacrit exceeding computed values. For μ = 0 and smaller η, comparison to experiment (with smaller aspect ratios) at low Re is slightly less good. For η = 0.77 and a range of μ, agreement with experiment is very good for Re 〈 135 except at the most positive or negative μ (where Taexptcrit 〉 Tacompcrit), whereas for Re ≥ 166, Taexptcrit 〉 Tacompcrit for all but the most positive μ. For η = 0.9497 and 0.959 and all but the most extreme values of μ, agreement is excellent (generally within 2%) up to the largest Re considered experimentally (200), again suggesting that finite-amplitude instability is unimportant. © 2004 Cambridge University Press.
    Print ISSN: 0022-1120
    Electronic ISSN: 1469-7645
    Topics: Mechanical Engineering, Materials Science, Production Engineering, Mining and Metallurgy, Traffic Engineering, Precision Mechanics , Physics
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  • 3
    Publication Date: 2004-06-25
    Description: For spiral Poiseuille flow with radius ratio η ≡ Ri/Ro = 0.5, we have computed complete linear stability boundaries for several values of the rotation rate ratio μ ≡ Ωo/Ωi, where Ri and Ro are the inner and outer cylinder radii, respectively, and Ωi and Ωo are the corresponding (signed) angular speeds. The analysis extends the previous range of Reynolds number Re studied computationally by more than eightyfold, and accounts for arbitrary disturbances of infinitesimal amplitude over the entire range of Re for which spiral Poiseuille flow is stable for some range of the Taylor number Ta. We show how the centrifugally driven instability (beginning with steady or azimuthally travelling-wave bifurcation of circular Couette flow at Re = 0 when μ 〈 η2) connects, as conjectured by Reid (1961) in the narrow-gap limit, to a non-axisymmetric Tollmien-Schlichting-like instability of non-rotating annular Poiseuille flow at Ta = 0. For μ 〉 η2, we show that there is no instability for 0 ≤ Re ≤ Remin. For μ = 0.5, Remin corresponds to a turning point, beyond which exists a range of Re for which there are two critical values of Ta, with spiral Poiseuille flow being stable below the lower one and above the upper one, and unstable in between. For the special case μ = 1, with the two cylinders having the same angular velocity, Remin corresponds to a vertical asymptote smaller than found by Meseguer & Marques (2002), whose results for μ 〉 η2 fail to account for disturbances with a sufficiently wide range of azimuthal wavenumbers. © 2004 Cambridge University Press.
    Print ISSN: 0022-1120
    Electronic ISSN: 1469-7645
    Topics: Mechanical Engineering, Materials Science, Production Engineering, Mining and Metallurgy, Traffic Engineering, Precision Mechanics , Physics
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