Abstract
The stability of a thin layer of liquid moving in still air is studied theoretically with the object of throwing light on the break-up of films during atomization. It is found that instability occurs if W = T/ρ 1U2h < 1 and that the wavelength for maximum growth factor, for W « 1, is λ = (4πT/ρ2U2) where ρ1 is the liquid density, ρ2 is the air density, U is the film velocity, 2h is the film thickness and T is the surface tension of the liquid. Comparison with experimental data shows fair agreement with the observed wavelengths.
Cite
CITATION STYLE
Squire, H. B. (1953). Investigation of the instability of a moving liquid film. British Journal of Applied Physics, 4(6), 167–169. https://doi.org/10.1088/0508-3443/4/6/302
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