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  • 1
    ISSN: 1476-4687
    Source: Nature Archives 1869 - 2009
    Topics: Biology , Chemistry and Pharmacology , Medicine , Natural Sciences in General , Physics
    Notes: [Auszug] The laboratory plasma is produced by transverse r.f. excitation of Argon gas in a 1-m long, 15-cm diameter, glass tube immersed in an axial magnetic field variable from 20 to 200 gauss, and uniform to within 2% over 60cm length. This method of plasma production4-5 creates a plasma with electron ...
    Type of Medium: Electronic Resource
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  • 2
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Physics of Fluids 6 (1994), S. 595-604 
    ISSN: 1089-7666
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The renormalization group theory of fluid turbulence is developed from a statistical mechanical viewpoint using an exact expression for the functional probability distribution of the velocity field. The latter is similar in form to an equilibrium Gibbs distribution, and is derived by combining Lagrangian statistical mechanics with an Eulerian fluid description. It is shown that this distribution enables an RG transformation to be defined, evaluated, and analyzed using statistical mechanical techniques. The method of determining amplitudes used here also differs from previous work, in that the indeterminacy of the relevant stirring force parameters is resolved through the essential requirement that all coarse-grained distributions must yield the actual dissipation rate E. Consequently, although the fixed point solutions of the dynamic RG approach are recovered, slightly different numerical results are obtained for amplitudes. The present approach yields, for example, for Kolmogorov's constant, CK=1.44.
    Type of Medium: Electronic Resource
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  • 3
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Physics of Fluids 6 (1994), S. 3750-3764 
    ISSN: 1089-7666
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The use of the turbulence renormalization group (RG) to calculate the constants occurring in the standard k-cursive-epsilon equations has yielded a low value for von Kármán's constant. A derivation of the turbulence transport equations is presented which addresses this problem from a new perspective based on a statistical mechanical RG. Different fixed points are used to describe the qualitatively different degrees of freedom associated with the various moment closures required. Initiation of the iteration of a particular moment in the correct domain of attraction is controlled by its effective initial value, the definition of which is embodied in the statistical mechanical RG. The conjectured singular contributions to the turbulence production and destruction of dissipation terms are calculated and their cancellation demonstrated. The finite residue yields the coefficient of the destruction of dissipation term. Only the "mixed'' term contributes to the coefficient of the production of dissipation term. For the logarithmic region of a turbulent boundary layer, the present approach yields 0.39 for von Kármán's constant and 3.2 for the shear parameter.
    Type of Medium: Electronic Resource
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  • 4
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Physics of Fluids 7 (1995), S. 2785-2795 
    ISSN: 1089-7666
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The probability distribution function (PDF), P(Δur), of a velocity difference, Δur, over a distance r in incompressible fluid turbulence is derived from the Navier–Stokes equations using the underlying functional probability distribution. Two different types of approximation are used to evaluate the resulting functional integral for P(Δur). The first is based on the saddle-point technique. It is used to examine the non-Gaussian features of P(Δur) and to demonstrate, in particular, that its tail has the characteristic exponential form associated with intermittency. The second approximation is developed for the purpose of deriving the anomalous scaling exponents of the structure functions from P(Δur). It represents P(Δur) as the integral with respect to the spatially averaged dissipation rate, εr, of the product of the PDF of Δur conditioned to a particular εr, and the PDF of εr. These are coarse-grained PDFs, obtained using the renormalization group. The former is approximately Gaussian, whereas the latter is given by a constrained Gaussian functional integral, which is evaluated approximately using a transformation that enables it to be represented in terms of a Poisson process. This approach yields the scaling exponents in the form discussed by She and Léveˆque [Phys. Rev. Lett. 72, 336 (1994)], and also gives the complete third-order structure function exactly. © 1995 American Institute of Physics.
    Type of Medium: Electronic Resource
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