jetstabilitet

Jetstabilitet refers to the behavior of a liquid jet as it propagates through a surrounding medium, and to the conditions under which the jet maintains a coherent column rather than breaking up into droplets. A stable jet remains slender over a given distance; an unstable jet develops perturbations on its surface that grow with time and can lead to disintegration.

Stability depends on jet radius R, mean velocity U, liquid density rho and viscosity mu, surface tension sigma, and properties of the surrounding medium (density rho_a and viscosity mu_a). Dimensionless numbers commonly describe these effects, such as the Reynolds number Re = rho U R / mu, the Weber number We = rho U^2 R / sigma, the Capillary number Ca = mu U / sigma, and the Ohnesorge number Oh = mu / sqrt(rho sigma R).

Two main instability mechanisms are often discussed: the capillary (Plateau–Rayleigh) instability, in which surface tension amplifies axisymmetric perturbations and tends to pinch the jet into droplets; and the Kelvin–Helmholtz instability, driven by shear between the jet and the surrounding fluid, which can generate waves on the interface and promote breakup at high speeds. Viscosity generally damps perturbations, stabilizing the jet and shifting the most unstable wavelength; electric or magnetic fields can also modify stability in electrohydrodynamic or magnetohydrodynamic contexts.

Linear stability analysis of a cylindrical jet yields a dispersion relation linking perturbation growth rate to wavenumber; for inviscid jets the most unstable wavelength is about 9 times the jet radius. In practice, jet stability is crucial for technologies such as inkjet printing, fuel injection, and spray formation, where control is achieved by adjusting flow rate, nozzle size, fluid properties, ambient pressure, or applying stabilizing fields.