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e - Propulsion and Combustion Laboratory

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Combined Heat Transfer – Formulations‣ Assumptions• The gas flow is incompressible <strong>and</strong> has constant properties.• Viscous work is negligible.• The gray gas absorbs, emits, <strong>and</strong> scatters radiation isotropically.• The wall is isothermal, <strong>and</strong> diffusely emits <strong>and</strong> reflects radiation.• The inflow is fully developed, <strong>and</strong> its temperature is uniform* *‣ Governing Equations ∇⋅ V = 0 1 ( V * ⋅∇ * ) V * = −∇ * p * + ∇*2 V*2 Re* * 1 *2 1 τ0 ⎛ 4 1 ⎞( V ⋅∇ ) Θ= ∇ Θ− ( 1 −ω0) ⎜Θ − GdΩ⎟RePr RePr N4Ω= 4π⎝∫⎠* * * *where x = x L, y = y L, u = u u0, v = v u0, τ0= β0L, ω0 = σsβ0T p − p* ref ρ0uLC0p0µ0Θ= , p = ,Re = ,Pr=2Twρ0u0 µ0k0k0β0IN = , G=3 44σTw σTw‣ Dimensionless RTE 1 dG( r , s ) 1 −ω4 ω =− Grs ( , ) + 0 Θ ( r) + 0 Grs ( , ′) Φ( ssd ′,) Ω′τ dsπ 4π ∫Ω=′ 4π0y(0,1)INLET(0,0)SYMMETRY PLANEy (x)=1.0(Re/3,1)HOT WALL (Re/3, y (Re/3))ly (x)=[tanh(2-30x/Re)-tanh(2)]/2‣ Source Term Linearization*2 2* ⎛ dS ⎞ * ⎡ 4 τ0 *3 ⎤ ⎡ 1 τ0⎛ *4 1 ⎞⎤S = S + ⎜ * ( Θ−Θ ) = − ( 1−ω0) Θ Θ + ( 1−ω0)⎜3Θ + GdΩ ⎟ = S Θ + SdΘ ⎟ ⎢RePr N⎥ ⎢RePr N 4Ω= 4π⎥⎝∫⎝ ⎠ ⎣ ⎦ ⎣ ⎠⎦T T P P P P P P CPl33 <strong>Propulsion</strong> <strong>and</strong> <strong>Combustion</strong> Lab.xy (x)luEXIT

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