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The Navier–Stokes equations (/nævˈjeɪ ˈstoʊks/ nav-YAY STOHKS) describe the motion of viscous fluids. This system of partial differential equations was named after Claude-Louis Navier and George Gabriel Stokes, who developed them over a few decades of progressive work, from 1822 (Navier) to 1842–1850 (Stokes). Siméon Denis Poisson independently achieved…
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equations displaystyle stokes navier equation flow fluid velocity mathbf left textstyle right pressure frac nabla partial incompressible cdot rho mu
| Subject | Predicate | Object | Confidence | Src |
|---|---|---|---|---|
| Navier–Stokes equations | is a | second most commonly seen | 0.90 | text |
| sound absorption | instance of | that is whenever we are not dealing with processes | 0.80 | text |
| attenuation of shock waves | instance of | that is whenever we are not dealing with processes | 0.80 | text |
| where second viscosity coefficient becomes important | instance of | that is whenever we are not dealing with processes | 0.80 | text |
| the Reynolds-averaged Navier | instance of | time-averaged equations | 0.80 | text |
| atoms or molecules | instance of | it is infinitely divisible and not composed of particles | 0.80 | text |
| Navier–Stokes equations | related to A three-dimensional steady-state vortex solution | Hopf | 0.60 | section |
| Navier–Stokes equations | related to A three-dimensional steady-state vortex solution | Let | 0.60 | section |
| Navier–Stokes equations | related to A three-dimensional steady-state vortex solution | One | 0.60 | section |
| Navier–Stokes equations | related to A three-dimensional steady-state vortex solution | This | 0.60 | section |
| Navier–Stokes equations | related to A three-dimensional steady-state vortex solution | Note | 0.60 | section |
| Navier–Stokes equations | related to A three-dimensional steady-state vortex solution | Clay Millennium | 0.60 | section |
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