메뉴 건너뛰기




Volumn 81, Issue 4, 2010, Pages

Dynamics of a two-dimensional vapor bubble confined between superheated or subcooled parallel plates

Author keywords

[No Author keywords available]

Indexed keywords

ANALYTICAL TREATMENT; CONSTANT VELOCITIES; CRITICAL VALUE; FAST MODE; FINITE LENGTH; FINITE TIME; INFINITE TIME; LOW PRANDTL NUMBER; PARALLEL PLATES; SLOW MODE; SMALL GAPS; SUBCOOLINGS; THIN LIQUID FILM; VAPOR BUBBLE; WAITING-TIME;

EID: 77951596853     PISSN: 15393755     EISSN: 15502376     Source Type: Journal    
DOI: 10.1103/PhysRevE.81.046314     Document Type: Article
Times cited : (5)

References (19)
  • 2
    • 84855585199 scopus 로고
    • 10.1017/S0022112061000160
    • F. P. Bretherton, J. Fluid Mech. 10, 166 (1961). 10.1017/ S0022112061000160
    • (1961) J. Fluid Mech. , vol.10 , pp. 166
    • Bretherton, F.P.1
  • 6
    • 32644452834 scopus 로고    scopus 로고
    • 10.1146/annurev.fluid.38.050304.092033
    • V. S. Ajaev and G. M. Homsy, Annu. Rev. Fluid Mech. 38, 277 (2006). 10.1146/annurev.fluid.38.050304.092033
    • (2006) Annu. Rev. Fluid Mech. , vol.38 , pp. 277
    • Ajaev, V.S.1    Homsy, G.M.2
  • 8
    • 56949092634 scopus 로고    scopus 로고
    • 10.1016/j.ijheatmasstransfer.2008.06.031
    • G. Wang and P. Cheng, Int. J. Heat Mass Transfer 52, 79 (2009). 10.1016/j.ijheatmasstransfer.2008.06.031
    • (2009) Int. J. Heat Mass Transfer , vol.52 , pp. 79
    • Wang, G.1    Cheng, P.2
  • 10
    • 1842575593 scopus 로고    scopus 로고
    • 10.1016/j.ijheatfluidflow.2003.11.005
    • J. R. Thome, Int. J. Heat Fluid Flow 25, 128 (2004). 10.1016/j. ijheatfluidflow.2003.11.005
    • (2004) Int. J. Heat Fluid Flow , vol.25 , pp. 128
    • Thome, J.R.1
  • 13
    • 77951591538 scopus 로고    scopus 로고
    • Ph.D. Thesis, Northwestern University
    • C. H. Panzarella, Ph.D. Thesis, Northwestern University, 1998 (unpublished).
    • (1998)
    • Panzarella, C.H.1
  • 15
    • 77951556526 scopus 로고    scopus 로고
    • www.comsol.com
  • 17
    • 77951603310 scopus 로고    scopus 로고
    • In the special case of equal superheating (i.e., when Δ Tu =Δ Tl =1) the argument of the logarithm in Eq. is multiplied by a factor of 2.
    • In the special case of equal superheating (i.e., when Δ T u = Δ T l = 1) the argument of the logarithm in Eq. is multiplied by a factor of 2.
  • 18
    • 77951575904 scopus 로고    scopus 로고
    • /2 in the present Eq. recovers the corrected version of their Eq. (59) when the different definitions of β are taken into account. Since D now appears only in the corrected version of their Eq. (59) in the combination β/D the solution for β in this case is simply β=0.7799D for all values of D. Fortunately, the qualitative conclusions of WDB's stability analysis are not affected by this minor error.
    • / 2 in the present Eq. recovers the corrected version of their Eq. (59) when the different definitions of β are taken into account. Since D now appears only in the corrected version of their Eq. (59) in the combination β / D the solution for β in this case is simply β = 0.7799 D for all values of D. Fortunately, the qualitative conclusions of WDB's stability analysis are not affected by this minor error.
  • 19
    • 77951568630 scopus 로고    scopus 로고
    • -4 ) are possible depending on a variety of factors including the local temperature and pressure and whether the free surface is stagnant or dynamically renewing, and so the value α=1 used here may significantly overestimate the local mass flux.
    • - 4) are possible depending on a variety of factors including the local temperature and pressure and whether the free surface is stagnant or dynamically renewing, and so the value α = 1 used here may significantly overestimate the local mass flux.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.