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hydrodynamics of a rotating strongly interacting fermi gas
hydrodynamics of a rotating strongly interacting fermi gas

A conservative and non-oscillatory scheme for Vlasov code simulations Takayuki Umeda
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... metric instability and an oscillatory ‘‘whipping’’ instability of the centerline of the jet; however, the quantitative characteristics of these instabilities disagree strongly with experiments. As an example, a water jet with a radius of order that used in Taylor’s 1969 experiments29 is predicted to ...
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... to the low collisionality of the plasma, kinetic modeling is mandatory for the study of tokamak turbulence. In principle, this implies the modeling of a six-dimensional distribution function representing the density of particles in position and velocity phase-space, which can be reduced to five dime ...
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[PDF]

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... To eliminate some constants we introduce atomic units. To get rid of the constants we • measure mass in me = 1a.u. (atomic unit). • measure charge in units of e = 1a.u.. • measure angular momentum in units of ~ = 1a.u. • measure permittivity of 4πo = 1a.u. In short atomic units, a.u. are defined by ...
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... Hodge star operators and take into account the case when circumcenters fall outside triangles or tetrahedrons, which may lead to negative dual volume without Delaunay triangulation. Then we demonstrate the implementation of various boundary conditions, including perfect magnetic conductor (PMC), per ...
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Derivation of the Navier–Stokes equations

The intent of this article is to highlight the important points of the derivation of the Navier–Stokes equations as well as the application and formulation for different families of fluids.
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