Method and apparatus for variable exhaust nozzle exit area
US-2015354498-A1 · Dec 10, 2015 · US
US10366182B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-10366182-B2 |
| Application number | US-201514806373-A |
| Country | US |
| Kind code | B2 |
| Filing date | Jul 22, 2015 |
| Priority date | Jul 22, 2015 |
| Publication date | Jul 30, 2019 |
| Grant date | Jul 30, 2019 |
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Methods and apparatus to model thermal mixing for prediction of multi-stream flows are described. An example method includes determining characteristics of a nozzle of an aircraft; estimating momentum diffusion due to turbulence associated with the nozzle based on the determined characteristics; and estimating thermal diffusion due to the turbulence associated with the nozzle based on the estimated momentum diffusion, wherein the estimating of the thermal diffusion due to the turbulence is based on a spatially varying turbulent Prandtl number.
Opening claim text (preview).
What is claimed is: 1. A method, comprising: receiving, at a processor, characteristics of a nozzle of an aircraft to be tested, the characteristics input by a person via an interface, the characteristics including a shape of the nozzle; generating, via the processor, a domain representation of the nozzle based on the characteristics of the nozzle, the domain representation divided into a plurality of cells; estimating, via the processor, momentum diffusion due to turbulence associated with the nozzle based on the determined characteristics; estimating, via the processor, thermal diffusion due to the turbulence associated with the nozzle based on the estimated momentum diffusion and a spatially varying turbulent Prandtl number, wherein the spatially varying turbulent Prandtl number is calculated using the equation Pr τ = μ τ ∇ T 2 ρ u j ′ T ′ _ · ∇ j T , wherein μ τ is turbulent viscosity, T is static temperature, ρ is density, and u′ j T′ is a turbulent heat flux vector, and wherein the turbulent heat flux vector is calculated using the equations ρ u j ′ T ′ _ * = k / ɛ c 1 θ + 1 2 ( P k ɛ - 1 ) ( ρτ jm ∂ T ∂ x m - ( 1 - c 2 θ ) ρ u m ′ T ′ _ ( N - 1 ) ∂ u j ∂ x m - c 1 θ , w ( ρ
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