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In computational fluid dynamics, the k–omega (k–ω) turbulence model is a common two-equation turbulence model, that is used as an approximation for the Reynolds-averaged Navier–Stokes equations (RANS equations). The model attempts to predict turbulence by two partial differential equations for two variables, k and ω, with the first variable being the turbulence kinetic energy (k) while the second (ω) is the specific rate of dissipation (of the turbulence kinetic energy k into internal thermal energy).

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  • En la mecánica de fluidos computacional, el modelo de turbulencia k-omega (k-ω) es un común de dos ecuaciones, utilizado como cierre de las (ecuaciones NSPR). El modelo intenta predecir la turbulencia mediante dos ecuaciones diferenciales parciales de dos variables, k y ω, siendo la primera variable la y, la segunda, la razón específica de disipación (de la energía cinética de turbulencia k a energía térmica interna). (es)
  • In computational fluid dynamics, the k–omega (k–ω) turbulence model is a common two-equation turbulence model, that is used as an approximation for the Reynolds-averaged Navier–Stokes equations (RANS equations). The model attempts to predict turbulence by two partial differential equations for two variables, k and ω, with the first variable being the turbulence kinetic energy (k) while the second (ω) is the specific rate of dissipation (of the turbulence kinetic energy k into internal thermal energy). (en)
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  • En la mecánica de fluidos computacional, el modelo de turbulencia k-omega (k-ω) es un común de dos ecuaciones, utilizado como cierre de las (ecuaciones NSPR). El modelo intenta predecir la turbulencia mediante dos ecuaciones diferenciales parciales de dos variables, k y ω, siendo la primera variable la y, la segunda, la razón específica de disipación (de la energía cinética de turbulencia k a energía térmica interna). (es)
  • In computational fluid dynamics, the k–omega (k–ω) turbulence model is a common two-equation turbulence model, that is used as an approximation for the Reynolds-averaged Navier–Stokes equations (RANS equations). The model attempts to predict turbulence by two partial differential equations for two variables, k and ω, with the first variable being the turbulence kinetic energy (k) while the second (ω) is the specific rate of dissipation (of the turbulence kinetic energy k into internal thermal energy). (en)
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  • Modelo de turbulencia k-omega (es)
  • K–omega turbulence model (en)
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