Abstract

Slender-body theory is used to determine the approximate static shape of a conically ended dielectric drop in an electric field. The shape and the electric-field distribution follow from solution of a second-order nonlinear ordinary differential equation that can be integrated numerically or analytically. An analytic formula is given for the dependence of the equilibrium cone angle on the ratio, 6/e, of the dielectric constants of the drop and the surrounding fluid. A rescaling of the equations shows that the dimensionless shape depends only on a single combination of e/e and the ratio of electric stresses and interfacial tension. In combination with numerical solution of the equations, the rescaling also establishes that, to within logarithmic factors, there is a critical field Em-m for cone formation proportional to (e/e- 1)~5/12, at which the aspect ratio of the drop is proportional to (e/ë- 1)1/2. Drop shapes are computed for EOO > Emin. For EOO 3≥ Emin the aspect ratio of the drop is proportional to E> . Analogous results apply to a ferrofluid in a magnetic field.

Original languageEnglish (US)
Pages (from-to)329-347
Number of pages19
JournalProceedings of the Royal Society A: Mathematical, Physical and Engineering Sciences
Volume455
Issue number1981
DOIs
StatePublished - Jan 1 1999

All Science Journal Classification (ASJC) codes

  • Mathematics(all)
  • Engineering(all)
  • Physics and Astronomy(all)

Keywords

  • Conical ends
  • Dielectric liquids
  • Drop deformation
  • Electric fields
  • Taylor cones

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