Surface Effects in Ionic Winds

Specific boundary conditions are necessary for the collecting electrode and discharge electrode in ionic wind simulations.

Collecting Electrode

Assuming an infinitely fast neutralization of ions at the collecting electrode boundary, zero space charge density ρ (equivocal to zero molar concentration) is applied together with zero electric potential ϕ , as a boundary condition. The collecting electrode is assumed to be grounded.

Discharge Electrode

The visual critical electric field E S C , which is set as a boundary condition, can be computed by:

Figure 1. EQUATION_DISPLAY
E S C = A δ + B δ a
(4163)
where:
  • E S C is the critical electric field intensity at the start of the corona
  • A and B are empirical constants for air and a negative corona—which usually have values of 32.3 × 10 5 V/m and 0.846 × 10 5 V/m 1 / 2 respectively
  • δ is the relative density of air which is assumed to be δ = 1
  • a represents the local radius of the curvature of the electrode
Note

On symmetry plane boundaries, dependent variables are assumed to have a zero gradient in the direction normal to the boundary.

Dielectric Boundaries

At dielectric boundaries, such as plastic housings of ionic wind generators, where no neutralization of ions is assumed to occur, the flux of ions is zero.