Momentum and Heat Transfer Analogy (continued) For the solution,the function f must be the same u=f(x,y".Re) T'=f(x',y',Re.Pr) As we know, Nu= OT" =f(x,Rer.Pr) C,= 是R小 We conclude that ReL-Nu C 2Momentum and Heat Transfer Analogy (continued) For the solution, the function f must be the same. As we know, We conclude that   T  , ,Re ,Pr , ,Re * * * * * * L L f x y u f x y     L L y L s f f x y u V C ,Re Re 2 Re 2 2 * 0 * * 2          Nu  ,Re ,Pr * 0 * * * L y f x y T      C Nu L f  2 Re