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Show I I I I , , 1111111111 , II I I I I II , , I I I I I I 1/ " , I I I I I II , I 1/1111/111 I II II I I I I , , /1'111111/ I II II , I I I I , , I I 1/ I , I I I I I I I I II I , , ,, I I I', }," 'II I, II II I" '"I II I II I I I I 1111"'" I I I I I I' , , , II " , , I I I I I' ~' I I I I , , , I I I I I I I """'" I I ,I ,I I I I I jl/I/'''' I I , , I' I' 1/ 1/ I I , I I I I I II ") I , I I I I / , , I I "I" I \\ u: ~ ~ ~ : : : : t I I" I I' I I 1'1 , t I 1 I 1 1 1 I / / / / It I I " , , I ;'1/1111" I / / I I It II II t I I -/1/111""/ '" It II 'I I II "'-'1111""' " • I I I I II II I I I II I I II I II II' I I I' " , II , , 1'1 f· igure 9 . LIM mode l results for mixing and CO llllJlI ,' UOI1 in (1 planar turbulent Jet. showing (al left) the lime-evolving compula tiona l ' ur/ilc on whi ch the loca l integra l JIl oment eq u a ti ons are so lved, and (al righl) the velocity veclor field as obtaineel from the lime -evolving vorlicity fidel . The lim ' - 'vo lvin .~ moments a t l'Ve'I)' point OJl this s urface are compuled from the LIM equations. with Ih strain rat a al every poinL d eLe nnine cl frol11 the de/ o nnCltion or the surl~H'(' by the vorUelly fielel . These moments prociuce th(' consenl d scalar fi eld C,(x,r) and the 'J socia led Cellar en ergy clissipa lion fa te field 'VS 'VS( x,l) s hown In Fig. 10, from which chemical specie and reaction rat n lds :' 11('/1 8S those in Fi .~ , II ~lrc olJl<lilll'd Ii s ing thl' ,-; tr"lill di s:-- ip<lliull and I'eactlon layer mapping approach . |