The Deformation and Break-up of a Single Slender Liquid Drop in a Linear Shear Flow |
Contents
Chapter I | 8 |
An Inviscid Drop λ 0 in Zero Reynolds Number | 16 |
b The flow in the outer region | 22 |
6 other sections not shown
Common terms and phrases
Acrivos analysis analytic apparatus approximation asymptotic belt speed boundary conditions bubble Buckmaster 1973 capillary pressure centipoise constant corresponding creeping-flow equations critical shear rate critical value deformation curve density dimensionless groups dimensionless shear rate dispersed phase Doctor of Philosophy drop break-up drop deformation droplets effect of inertia experimental extensional flow figure finite flow field fluid Gua/y Gualy hence hyperbolic flow inertia inertial effects inner region inner solution integer integral interface interfacial tension internal viscosity inviscid drop kinematic condition liquid drop low Reynolds number maximum shear rate normal stress balance obtained parallel-band parameter prior to break-up R₁ radius reservoir shear stress simple shear flow singular region slender drop slender-body theory steady-state Stokes flow surface tension syrup test section Torza trichloroethylene undisturbed flow velocity viscosity ratio