A very short ripple on the surface of water is controlled by surface tension rather…

PHYSICS · Multi-part · Fermi University Physics · Scientific Practice & Experimental Methods · Oscillations, Waves & Acoustics · Quantities, units and the practice of measurement

Measurement and Method, Ch What dimensions decide before you measure anything

Problem

A very short ripple on the surface of water is controlled by surface tension rather than gravity. The relevant quantities are judged to be the surface tension σ\sigma (unit N m−1\mathrm{N\,m^{-1}}), the density of water ρm\rho_{\rm m} (unit kg m−3\mathrm{kg\,m^{-3}}), and the wavelength λ\lambda (unit m\mathrm{m}). ((a)) Write the ripple speed as v=Cσαρmβλγv = C\sigma^{\alpha}\rho_{\rm m}^{\beta}\lambda^{\gamma} with CC dimensionless, and use dimensional homogeneity to find α\alpha, β\beta and γ\gamma. ((b)) For water at 20 ∘C20\ ^\circ\mathrm{C}, with σ=0.0728 N m−1\sigma = 0.0728\ \mathrm{N\,m^{-1}} and ρm=998 kg m−3\rho_{\rm m} = 998\ \mathrm{kg\,m^{-3}}, and for a ripple of wavelength λ=2.0 mm\lambda = 2.0\ \mathrm{mm}, evaluate vv in terms of CC. ((c)) Wave theory (not this method) gives C=2πC = \sqrt{2\pi} for this ripple. State the numerical speed to two significant figures.

Browse the problem library