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  • 1
    Electronic Resource
    Electronic Resource
    Hoboken, NJ : Wiley-Blackwell
    AIChE Journal 38 (1992), S. 1675-1682 
    ISSN: 0001-1541
    Keywords: Chemistry ; Chemical Engineering
    Source: Wiley InterScience Backfile Collection 1832-2000
    Topics: Chemistry and Pharmacology , Process Engineering, Biotechnology, Nutrition Technology
    Additional Material: 1 Ill.
    Type of Medium: Electronic Resource
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  • 2
    Publication Date: 1992-10-01
    Print ISSN: 0001-1541
    Electronic ISSN: 1547-5905
    Topics: Chemistry and Pharmacology , Process Engineering, Biotechnology, Nutrition Technology
    Published by Wiley on behalf of American Institute of Chemical Engineers.
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  • 3
    Electronic Resource
    Electronic Resource
    s.l. : American Chemical Society
    Langmuir 6 (1990), S. 1715-1724 
    ISSN: 1520-5827
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology
    Type of Medium: Electronic Resource
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  • 4
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 92 (1990), S. 5569-5579 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: A generalized formulation of the Fokker–Planck equation is utilized to calculate the mean velocity and dispersivity of a flexible Brownian cluster of rigid particles which is acted upon by a time-periodic external force. It is shown that if the force consists of a nonzero mean part and a "fluctuating'' (i.e., zero mean) part, their effects are decoupled. Similarly, if a Fourier expansion of the force is carried out, the effect of each term of the expansion can be treated independently of the others. A representative force term of the form Fn exp(iωnt) +Fˆn exp(−iωnt) was selected to act upon a flexible dumbbell composed of two identical tethered spheres of radii a, with the inextensible tether acting as an "attractive'' internal potential. The dispersion tensor is found to consist of a "parallel'' contribution (directed along FnFˆn+FˆnFn) and a "hydrostatic'' contribution. This dispersion tensor depends linearly upon the scalar (Fn⋅Fˆn)a/24πμkT (μ=viscosity), approaches a constant asymptotic value for small nondimensional frequencies Ωn=12πμa3ωn/kT, and decreases asymptotically to zero for very large frequencies.
    Type of Medium: Electronic Resource
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  • 5
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: A systematic perturbation solution scheme is developed for calculating the laterally averaged effective reaction velocity constant K* for a chemically reactive solute undergoing a laterally inhomogeneous chemical reaction within a laterally bounded (but longitudinally unbounded) domain through which the solute is transported by convection and diffusion. This is accomplished by use of a perturbation operator technique which is used to obtain a time-dependent effective reaction velocity constant via a systematic perturbation expansion about the nonreactive, purely convective–diffusive Taylor dispersion state. The generally nonequilibrium initial spatial solute distribution requires use of a "fictitious'' macroscale initial condition in the first-order macroscale linear decay law governing the total amount of solute present in the system at any time. This fictitious value differs from the true value of the total amount of solute initially present. Comparison is made between the present formalism and that developed by Wilemski-Fixman and others in the analysis of partially diffusion-controlled reactions of tracer corpuscles and polymers diffusing within laterally unbounded domains (from which convection is absent). An example drawn from this field confirms the viability of the scheme. Perturbative expressions are also derived for the mean tracer velocity vector U* and Taylor dispersion dyadic @SD* about this mean. The asymptotic expression obtained for the convective contribution to @SD* explicitly manifests the effect of the inhomogeneous chemical reaction upon this effective transport coefficient.
    Type of Medium: Electronic Resource
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  • 6
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 89 (1988), S. 7510-7520 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: A generalized Taylor dispersion analysis is presented of the combined diffusion and sedimentation of a Brownian particle subjected to a spatially periodic potential plus a uniform force. At long times this transport process is macroscopically characterized by a uniform mean drift velocity vector of the Brownian particle, and by a dispersion dyadic that quantifies stochastic "spreading'' about the (traveling) mean position. A general explicit integral formula is derived for the dispersion coefficient in the one-dimensional case, which supplements known results for the mean velocity. Illustrative calculations show that, for sufficiently large values of the drift force, the dispersivity exceeds the molecular diffusivity, which characterizes dispersion in the absence of any potential barriers. These calculations also lead to the surprising conclusion that an increase in the height of the potential barriers can sometimes lead to an increase in the dispersivity. A general asymptotic analysis is developed for the limiting case where the drift force tends to infinity. Although in one dimension the dominance of the drift force over the potential leads to a spatially uniform, steady-state, periodic distribution, the same behavior does not generally obtain in higher-dimensional cases. Asymptotic expressions are derived for the mean velocity and dispersivity characterizing one-dimensional systems and a class of two-dimensional systems. The analysis is subsequently applied to the related problem of sedimentation and dispersion of a particle within a medium for which its molecular diffusivity is a periodic function of position (in the absence of any potential). Although a periodic potential and a periodic diffusivity lead to equivalent mathematical problems in the absence of a sedimentation force, the presence of drift leads to important qualitative differences.
    Type of Medium: Electronic Resource
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  • 7
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 85 (1986), S. 5238-5245 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: A novel moment-gradient expansion scheme, expressing the microscale probability density P as an infinite sum of global-space gradients of its corresponding macroscale density P¯ multiplied by coefficients formed from its local and total moments, is employed to derive an asymptotic long-time macrotransport equation from its more detailed microtransport predecessor. Particular emphasis is paid to third- and higher-order gradient terms in the expansion. These are shown to result in non-Gaussian behavior of the macroscale probability density P¯ governing convective–diffusive transport processes.
    Type of Medium: Electronic Resource
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  • 8
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 85 (1986), S. 4038-4044 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The theory of macrotransport processes is extended to include systems that undergo first-order irreversible bulk and/or surface chemical reactions in confined geometries. A convective-diffusion type kinetic equation incorporating both bulk and surface reaction terms is assumed to describe the microtransport of a reactive tracer particle in a multidimensional phase space. The independent positional and configurational variables appearing therein are decomposed into local (fast) and global (slow) variables, the distinction between them being based upon the existence of a small dimensionless parameter ε appearing in a scaled form of the kinetic equation. Elimination of the fast variables via a systematic perturbation scheme in ε results in a kinetic equation that governs the macrotransport of the reactive tracer. Expressions are obtained for the three physical-space phenomenological coefficients appearing therein, namely the mean velocity vector U¯*, dispersivity dyadic D¯*, and reaction velocity constant K¯*, in terms of quadratures of the seven local-space coordinate-dependent microtransport phenomenological functions appearing in the original kinetic equation. These macrocoefficients are given both Eulerian and Lagrangian interpretations.
    Type of Medium: Electronic Resource
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  • 9
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 90 (2001), S. 6553-6554 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: In a recent article [J. Appl. Phys. 89, 4667 (2001)], Beard applies Taylor dispersion theory for two-dimensional Poiseuille flow between flat plates to analyze mixing processes occurring at the entrance of a microfluidic T sensor. The classical value of the coefficient of the Taylor dispersivity, 1/210, differs from Beard's result, and this Comment points out elements of Beard's derivation which lead to his erroneous value of 33/560. Moreover, the lateral boundedness of the actual device and the long-time asymptotic nature of Taylor dispersion theory call into question the use of the latter model in the context of the T sensor described in Beard's analysis. © 2001 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 10
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 84 (1986), S. 2801-2807 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Projection operator methods are used to derive a systematic perturbation expansion scheme that provides formal justification for the otherwise ad hoc arguments underlying generalized Taylor dispersion theory. The latter theory is a coarse-graining procedure for eliminating the internal variables from multidimensional phase-space convective-diffusion-type transport equations in the limit of long times. In addition to rationalizing the otherwise ad hoc Lagrangian moment scheme, projection operator methods are further used to: (i) investigate nonasymptotic effects arising from "memory'' of the initial conditions; (ii) establish the existence of higher-order contributions beyond second-order terms in the physical-space spatial gradients. Explicit criteria are developed for when these third- and higher-order non-Gaussian terms may be neglected in the coarse-grained, Taylor dispersion or macrotransport equation.
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