Difference between revisions of "Turbulent Advection of a Fluid Discontinuity and Schr?dinger Mechanics"
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==Abstract== | ==Abstract== | ||
| − | A particle is modeled by a conserved discontinuity - a void or phase precipitate - of a turbulent ideal fluid. A medium discontinuity is split and dispersed in the stochastic environment forming a gas without hydrostatic pressure. Two equal-mass fragments of a discontinuity are indistinguishible from each other. A gas that posesses such properties must behave like the Madelung medium[[Category:Scientific Paper]] | + | A particle is modeled by a conserved discontinuity - a void or phase precipitate - of a turbulent ideal fluid. A medium discontinuity is split and dispersed in the stochastic environment forming a gas without hydrostatic pressure. Two equal-mass fragments of a discontinuity are indistinguishible from each other. A gas that posesses such properties must behave like the Madelung medium |
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| + | [[Category:Scientific Paper|turbulent advection fluid discontinuity schr dinger mechanics]] | ||
Latest revision as of 11:34, 1 January 2017
| Scientific Paper | |
|---|---|
| Title | Turbulent Advection of a Fluid Discontinuity and Schr?dinger Mechanics |
| Author(s) | Valery P Dmitriyev |
| Keywords | passive scalar, aether discontinuity, quantum mechanics |
| Published | 1999 |
| Journal | Galilean Electrodynamics |
| Volume | 10 |
| Number | 5 |
| Pages | 95-99 |
Abstract
A particle is modeled by a conserved discontinuity - a void or phase precipitate - of a turbulent ideal fluid. A medium discontinuity is split and dispersed in the stochastic environment forming a gas without hydrostatic pressure. Two equal-mass fragments of a discontinuity are indistinguishible from each other. A gas that posesses such properties must behave like the Madelung medium
