Quick Recap — Fluid Dynamics, Surface Tension & Viscosity

  • Continuity: Av=A v= const, so v1A1r2v\propto\dfrac{1}{A}\propto\dfrac{1}{r^2}. Bernoulli: P+12ρv2+ρgh=P+\tfrac12\rho v^2+\rho g h= const (fast flow \Rightarrow low pressure).
  • Efflux (Torricelli): v=2ghv=\sqrt{2gh}.
  • Surface tension: excess pressure in a drop 2Tr\dfrac{2T}{r}, in a soap bubble 4Tr\dfrac{4T}{r}. Capillary rise h=2Tcosθrρgh=\dfrac{2T\cos\theta}{r\rho g} (so h1rh\propto\dfrac1r).
  • Surface energy =T×=T\timesarea; work to blow a soap bubble =8πr2T=8\pi r^2 T (two surfaces).
  • Viscosity: Stokes drag F=6πηrvF=6\pi\eta r v; terminal velocity vt=2r2(ρσ)g9ηv_t=\dfrac{2r^2(\rho-\sigma)g}{9\eta} (so vtr2v_t\propto r^2).

Worked mini-example. Water (T=0.072T=0.072 N/m) rises in a capillary of radius 0.20.2 mm: h=2Trρg=2×0.072(2×104)(1000)(10)=0.072h=\dfrac{2T}{r\rho g}=\dfrac{2\times0.072}{(2\times10^{-4})(1000)(10)}=0.072 m =7.2=7.2 cm.