Absolute and convective instability of a radially expanding liquid sheet

被引:27
|
作者
Lin, SP [1 ]
Jiang, WY [1 ]
机构
[1] Clarkson Univ, Dept Mech & Aeronaut Engn, Potsdam, NY 13699 USA
关键词
D O I
10.1063/1.1570422
中图分类号
O3 [力学];
学科分类号
08 ; 0801 ;
摘要
A radially expanding liquid sheet of a finite radius can be formed by impacting a liquid jet on a circular disk [Savart, Ann. Chim. Phys. 54, 55 (1833); Ann. Chim. 54, 113 (1833) or by impinging two jet heads on against each other [Savart, Ann. Chim. Phys. 55, 257 (1833)]. The breakup of the liquid sheet first observed by Savart at the outer rim of the sheet is explained from the point of view of absolute and convective instability. Whether the sheet is convectively or absolutely unstable depends on the local Weber number We=rhoU(2)H/S, where rho and S are, respectively, the liquid density and the surface tension, and H and U are, respectively, the local half-sheet thickness and the local average liquid velocity. It is shown that absolute instability occurs at We=1, and convective instability occurs in the region where We. l. In the radially expanding liquid sheet, H decreases inversely with the radial distance from the center of the sheet, but U remains constant. Thus, the local Weber number that is greater than one near the center must decrease radially, and eventually reaches one where the sheet encounters absolute instability. In absolute instability, the disturbance propagates upstream to terminate the liquid sheet. This is one of the two regimes of breakup. The onset of absolute instability in this regime always occurs at the broken free edge, where the local Weber number is 1, regardless of the sheet radius. Taylor [Proc. R. Soc. London, Ser. A 253, 296 (1959)] obtained the same criterion from a balance of the surface tension force with a time rate of change of momentum experienced by the fluid at the broken edge. In regime II, it is shown that the sheet may break up at local Weber numbers greater than 1, due to convective instability. The global implications of the local absolute instability are discussed in connection with the related phenomena of breakups of planar sheets, water bells and annular jets. (C) 2003 American Institute of Physics.
引用
收藏
页码:1745 / 1754
页数:10
相关论文
共 50 条
  • [31] THE CONVECTIVE AND ABSOLUTE INSTABILITY IN BOUNDED MEDIA
    FEDORCHENKO, AM
    RADIOTEKHNIKA I ELEKTRONIKA, 1982, 27 (09): : 1833 - 1835
  • [32] Absolute/convective instability of the Batchelor vortex
    Olendraru, C
    Sellier, A
    Rossi, M
    Huerre, P
    COMPTES RENDUS DE L ACADEMIE DES SCIENCES SERIE II FASCICULE B-MECANIQUE PHYSIQUE CHIMIE ASTRONOMIE, 1996, 323 (03): : 153 - 159
  • [33] OBSERVATION OF TRANSITION FROM A CONVECTIVE INSTABILITY TO AN ABSOLUTE INSTABILITY
    GARSCADD.A
    BLETZING.P
    BULLETIN OF THE AMERICAN PHYSICAL SOCIETY, 1968, 13 (02): : 300 - &
  • [34] Liquid sheet instability
    Mechanical Engineering Department, Tuskegee University, Tuskegee, AL 36088, United States
    Acta Mech, 3-4 (153-167):
  • [35] Liquid sheet instability
    Ibrahim, EA
    Akpan, ET
    ACTA MECHANICA, 1998, 131 (3-4) : 153 - 167
  • [36] Liquid sheet instability
    E. A. Ibrahim
    E. T. Akpan
    Acta Mechanica, 1998, 131 : 153 - 167
  • [37] THE DISTRIBUTION OF PERFORATIONS IN A RADIALLY THINNING LIQUID SHEET
    SPIELBAUER, TM
    AIDUN, CK
    TAPPI JOURNAL, 1994, 77 (09): : 95 - 102
  • [38] Convective and absolute electrokinetic instability with conductivity gradients
    Chen, CH
    Lin, H
    Lele, SK
    Santiago, JG
    JOURNAL OF FLUID MECHANICS, 2005, 524 : 263 - 303
  • [39] Absolute and Convective Instability of the African Easterly Jet
    Diaz, Michael
    Aiyyer, Anantha
    JOURNAL OF THE ATMOSPHERIC SCIENCES, 2015, 72 (05) : 1805 - 1826