09Class 11 Physics

Mechanical Properties of Fluids formulas

Pressure, flow and surface tension formulas for Mechanical Properties of Fluids. Most numericals here use Bernoulli and continuity together.

Pressure and buoyancy

Pressure at depth
p=p0+ρgh\displaystyle p = p_0 + \rho g h
Pascal's law (hydraulic lift)
F1A1=F2A2\displaystyle \frac{F_1}{A_1} = \frac{F_2}{A_2}
Archimedes' principle
Fb=ρfluid Vdisplaced g\displaystyle F_b = \rho_{\text{fluid}}\, V_{\text{displaced}}\, g

Flowing fluids

Continuity equation
A1v1=A2v2\displaystyle A_1v_1 = A_2v_2
Bernoulli's equation
p+12ρv2+ρgh=constant\displaystyle p + \tfrac12\rho v^2 + \rho g h = \text{constant}

For steady, incompressible, non-viscous flow.

Torricelli's law
v=2gh\displaystyle v = \sqrt{2gh}

Viscosity

Viscous force
F=ηAdvdx\displaystyle F = \eta A\frac{dv}{dx}
Stokes' law
F=6πηrv\displaystyle F = 6\pi\eta r v
Terminal velocity
vt=2r2(ρ−σ)g9η\displaystyle v_t = \frac{2r^2(\rho - \sigma)g}{9\eta}

ρ is the sphere's density and σ the fluid's.

Reynolds number
Re=ρvdη\displaystyle R_e = \frac{\rho v d}{\eta}

Surface tension

Surface tension
S=FL\displaystyle S = \frac{F}{L}
Excess pressure in a drop
Δp=2Sr\displaystyle \Delta p = \frac{2S}{r}
Excess pressure in a soap bubble
Δp=4Sr\displaystyle \Delta p = \frac{4S}{r}

A bubble has two surfaces.

Capillary rise
h=2Scos⁡θρgr\displaystyle h = \frac{2S\cos\theta}{\rho g r}

Where students slip up

  • Using 2S/r for a soap bubble. It has two surfaces, so it's 4S/r.
  • Applying Bernoulli to viscous flow, or between points on different streamlines.
  • Forgetting gauge pressure leaves out atmospheric pressure, while absolute pressure includes it.

Try it on your weakest chapter.

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