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κTakahashietal./ProceedingsoftheCombustionInstitute30(205)2271-2277 2277
[5] D.N. Schi1ler，H.D. Ross，W .A. Sirignaro，AIAA paper93-0285.
[6]A.Ito，A.Narumi，T.Konishi，G.Tashtoush，K. Saito，C.J. Cremers，よ Heat Transfer 121 (19 9 9) 413-419.
[7]T.Konishi，G.Tashtoush，A.Ito，A.Narumi，K. Saito，Proc.Combust.Inst.28(20)2819-2826. [8]T. Konishi，A. Ito，Y. Kudo，K.Saito，Proc.
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26(196)1319-1325.
[10JD.N. Schil ler，H.D. Ross，W.A. Sirignano，Com-
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Comment
MichaelDelichαtsios，University01Ulster，UK.How doyoudetermineh?Also，intheconservatiol). Eqs. (1， 2)thedepthoftheliquidH shouldreplaceh.
Reply.Thevalueh，asodatedwithsub-surfaceliquid circulation and experimental1y determined，is a key parameterinEqs.(1， 2).Thisisoneofthemajorconclu- sionsinourpaper.Inthepast，thedepthofliquidwasused
[l1JF.A.Wiliams，CombustionTheory，seconded.1985， Benjamin/Cummings，MenloPark，CA，Chapter12. [12JT. Fukano，A.Ito，A. Ousaka，Physicochem.
Hydrodyn.6(1-2)(1985)23-47. [13JA.Ito，H.Kawano，T.Fukano，JSMBInt.J.35(4)
(192)565-572.
[14JK. Takahashi，A. Ito，Y. Kudo，T. Konishi，K.
Saito，Procedings 01the Fourth International $ymposium on Scαle Modeling，Cleveland，O H， September203.
[15]K.Akita，Proc.Combust.Inst.14(1973)1075-1083. [16]Y. Matsumoto，T. Saito，Bul l. JSMB 24 (1981)
160-167.
inthegoverningequationsasyoupointedout(Ref.[1Jin paper)，becausethedetailedthermalandfiuiddynamic structuresintheliquidphasewerenotwelunderstod. Weexperimental1ymeasuredthesestructures，andfound hasamoreacuratecharacteristiclengththantheliquid depth.Wealsofoundthatthevaluehcanbeusedtosep- aratethethickliquidpolfromthethinliquidpolcondi- tion，anotherbenefitasshowninFig.5.
