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Basic equations for suspension flows with interphase mass-transfer
Liu DY(刘大有); Wang BY(王柏懿); LIU, DY (reprint author), ACAD SINICA,INST MECH,BEIJING 100080,PEOPLES R CHINA.
Source PublicationScience in China Series A-Mathematics Physics Astronomy & Technological Sciences
1991
Volume34Issue:2Pages:166-180
ISSN1001-6511
AbstractIn the case of suspension flows, the rate of interphase momentum transfer M(k) and that of interphase energy transfer E(k), which were expressed as a sum of infinite discontinuities by Ishii, have been reduced to the sum of several terms which have concise physical significance. M(k) is composed of the following terms: (i) the momentum carried by the interphase mass transfer; (ii) the interphase drag force due to the relative motion between phases; (iii) the interphase force produced by the concentration gradient of the dispersed phase in a pressure field. And E(k) is composed of the following four terms, that is, the energy carried by the interphase mass transfer, the work produced by the interphase forces of the second and third parts above, and the heat transfer between phases. It is concluded from the results that (i) the term, (-alpha-k-nabla-p), which is related to the pressure gradient in the momentum equation, can be derived from the basic conservation laws without introducing the "shared-pressure presumption"; (ii) the mean velocity of the action point of the interphase drag is the mean velocity of the interface displacement, upsilonBAR-i. It is approximately equal to the mean velocity of the dispersed phase, upsilonBAR-d. Hence the work terms produced by the drag forces are f(dc) . upsilonBAR-d, and f(cd) . upsilonBAR-d, respectively, with upsilonBAR-i not being replaced by the mean velocity of the continuous phase, upsilonBAR-c; (iii) by analogy, the terms of the momentum transfer due to phase change are upsilonBAR-d-GAMMA-c, and upsilonBAR-d-GAMMA-d, respectively; (iv) since the transformation between explicit heat and latent heat occurs in the process of phase change, the algebraic sum of the heat transfer between phases is not equal to zero. Q(ic) and Q(id) are composed of the explicit heat and latent heat, so that the sum Q(ic) + Q(id)) is equal to zero.
KeywordInteractions Between Phases Suspension Flows Shared-pressure Presumption
Indexed BySCI
Language英语
WOS IDWOS:A1991FK38900005
WOS Research AreaMathematics
WOS SubjectMathematics, Applied ; Mathematics
Citation statistics
Cited Times:1[WOS]   [WOS Record]     [Related Records in WOS]
Document Type期刊论文
Identifierhttp://dspace.imech.ac.cn/handle/311007/39544
Collection力学所知识产出(1956-2008)
Corresponding AuthorLIU, DY (reprint author), ACAD SINICA,INST MECH,BEIJING 100080,PEOPLES R CHINA.
Recommended Citation
GB/T 7714
Liu DY,Wang BY,LIU, DY . Basic equations for suspension flows with interphase mass-transfer[J]. Science in China Series A-Mathematics Physics Astronomy & Technological Sciences,1991,34,2,:166-180.
APA 刘大有,王柏懿,&LIU, DY .(1991).Basic equations for suspension flows with interphase mass-transfer.Science in China Series A-Mathematics Physics Astronomy & Technological Sciences,34(2),166-180.
MLA 刘大有,et al."Basic equations for suspension flows with interphase mass-transfer".Science in China Series A-Mathematics Physics Astronomy & Technological Sciences 34.2(1991):166-180.
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