Similarity Solution(cont.) Subject to prescribed boundary conditions,numerical solutions to the momentum and energy equations yield the following results for important local boundary layer parameters: with u/u =0.99 at n=5.0, 5.0 5x 6= 1/2 (Re,)v2 with ,yl Bu =uuu。/x dn 7=0 and df1dnl。=0.332, C.=2=064Re pu12 -with h.=gg1(.亿-T)=kaT'/a,。=k(u./w)dr'/d切，o and dTd.332 P for Pr.6 =0.332Re2prv3 and Nus=k =Prl/3Similarity Solution (cont.) • Subject to prescribed boundary conditions, numerical solutions to the momentum and energy equations yield the following results for important local boundary layer parameters: ( ) ( ) 1/2 1/2 - with / 0.99 at 5. 5.0 5 / 0, Rex x u vx u u η δ ∞ ∞ = = = = 2 2 0 0 - with / s y u d f u u vx y d η τμ μ η ∞ ∞ = = ∂ = = ∂ 2 2 0 and / 0.332, df d η η = = , 1/2 , 2 0.664Re / 2 x s x Cf x uτρ − ∞ ≡ = ( ) ( ) * * 1/2 0 0 - with / / / / xss y h q T T k T y k u vx dT d η ∞ ∞ η = = = − =∂ ∂ = ′′ * 1/3 0 and / 0.332 Pr for Pr 0.6, dT d η η = = > 1/2 1/3 0.332 Re Pr x x x h x Nu k = = 1/3 r and P t δ δ =