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| Smoothed Particle Hydrodynamics× | 直接数値シミュレーション× | |
|---|---|---|
| 分野 | 流体力学 | 流体力学 |
| 系統 | Process / pipeline | Process / pipeline |
| 提唱年≠ | 1977 | 1971 |
| 提唱者≠ | Monaghan John & Lucy Leon | Steven Orszag |
| 種類≠ | Meshfree particle method | Full-scale turbulence resolution method |
| 原典≠ | Lucy, L. B. (1977). A numerical approach to the testing of the fission hypothesis. The Astronomical Journal, 82(12), 1013-1024. DOI ↗ | Orszag, S. A. (1971). Numerical simulation of incompressible flows within simple boundaries: accuracy. Journal of Fluid Mechanics, 49(1), 75-112. DOI ↗ |
| 別名 | SPH, particle hydrodynamics | DNS, resolved turbulence simulation |
| 関連 | 5 | 5 |
| 概要≠ | Smoothed Particle Hydrodynamics (SPH) is a meshfree particle method for simulating fluid dynamics, developed independently by Lucy in 1977 and Gingold and Monaghan in 1977. Rather than discretizing on a fixed grid, SPH represents fluids as collections of particles that carry mass, momentum, and energy. Each particle interacts with neighbors within a kernel support radius, enabling natural handling of free surfaces, large deformations, and multiphase flows without remeshing. SPH has become indispensable for simulations involving violent flows, impacts, and complex interfaces. | Direct Numerical Simulation (DNS) is a computational approach that solves the Navier-Stokes equations without turbulence models, resolving all scales of motion from the largest energy-containing eddies down to the smallest dissipative scales (Kolmogorov microscales). Pioneered by Steven Orszag in 1971, DNS provides complete information about turbulent flow fields and serves as a reference solution for validating turbulence models. However, extreme computational demands limit DNS to relatively simple geometries and low to moderate Reynolds numbers. |
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