A ripple tank is filled to a depth of with silicone oil of density and surface tension

PHYSICS · Multi-part · Fermi University Physics · Fluids & Continuum Physics · Waves, acoustics and compressible flow · Waves, acoustics and compressible flow

Fluids and Continuum Physics, Ch Surface gravity and capillary waves

Problem

A ripple tank is filled to a depth of 0.25 m0.25\ \mathrm{m} with silicone oil of density ρ=960 kg m−3\rho = 960\ \mathrm{kg\,m^{-3}} and surface tension γ=0.021 N m−1\gamma = 0.021\ \mathrm{N\,m^{-1}}. Take g=9.8 m s−2g = 9.8\ \mathrm{m\,s^{-2}}, treat the oil as inviscid and incompressible and the waves as small-amplitude and irrotational. ((a)) Find the minimum possible phase speed of a wave on this oil surface and the wavelength at which it occurs, quoting the capillary length ℓc=γ/(ρg)\ell_c = \sqrt{\gamma/(\rho g)}. ((b)) A vertical wire of diameter 1.0 mm1.0\ \mathrm{mm} is drawn through the surface at 0.40 m s−10.40\ \mathrm{m\,s^{-1}}. Compute the Weber number We=ρU2d/γ\mathrm{We} = \rho U^{2} d/\gamma of the wire, using the wire diameter dd as the length scale. ((c)) The tank also carries a wave of wavelength 0.30 m0.30\ \mathrm{m} and amplitude 4.0 mm4.0\ \mathrm{mm}. Show that at this wavelength the wave is a deep-water gravity wave (surface tension negligible), and find its phase speed and the energy flux per metre of crest.

Browse the problem library