Viscosity — Stokes law and terminal velocity of a sphere falling in fluid

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Question

A steel ball of radius 2 mm and density 8000 kg/m³ falls through glycerine of density 1300 kg/m³ and viscosity 0.83 Pa·s. Find the terminal velocity using Stokes' law. Also derive the expression for terminal velocity.

(JEE Main 2022, similar pattern)


Solution — Step by Step

Forces on the sphere

Three forces act on a sphere falling through a viscous fluid:

  1. Weight (downward): W=43πr3ρsgW = \frac{4}{3}\pi r^3 \rho_s g
  2. Buoyancy (upward): Fb=43πr3ρfgF_b = \frac{4}{3}\pi r^3 \rho_f g
  3. Viscous drag (upward): Fv=6πηrvF_v = 6\pi \eta r v (Stokes' law)

where ρs\rho_s = density of sphere, ρf\rho_f = density of fluid, η\eta = viscosity.

Derive terminal velocity

At terminal velocity, acceleration = 0. So net force = 0:

W=Fb+FvW = F_b + F_v

43πr3ρsg=43πr3ρfg+6πηrvt\frac{4}{3}\pi r^3 \rho_s g = \frac{4}{3}\pi r^3 \rho_f g + 6\pi \eta r v_t

6πηrvt=43πr3(ρsρf)g6\pi \eta r v_t = \frac{4}{3}\pi r^3 (\rho_s - \rho_f) g

Terminal Velocity

vt=2r2(ρsρf)g9ηv_t = \frac{2r^2(\rho_s - \rho_f)g}{9\eta}

Substitute numerical values

r=2×103r = 2 \times 10^{-3} m, ρs=8000\rho_s = 8000 kg/m³, ρf=1300\rho_f = 1300 kg/m³, η=0.83\eta = 0.83 Pa·s, g=9.8g = 9.8 m/s².

vt=2×(2×103)2×(80001300)×9.89×0.83v_t = \frac{2 \times (2 \times 10^{-3})^2 \times (8000 - 1300) \times 9.8}{9 \times 0.83}

=2×4×106×6700×9.87.47= \frac{2 \times 4 \times 10^{-6} \times 6700 \times 9.8}{7.47}

=2×4×6700×9.8×1067.47=525280×1067.47= \frac{2 \times 4 \times 6700 \times 9.8 \times 10^{-6}}{7.47} = \frac{525280 \times 10^{-6}}{7.47}

vt0.0703 m/s7.03 cm/sv_t \approx \mathbf{0.0703 \text{ m/s}} \approx 7.03 \text{ cm/s}


Why This Works

When a sphere enters a viscous fluid, it initially accelerates due to gravity. But the viscous drag increases with velocity (Stokes' law: FvF \propto v). Eventually, the drag + buoyancy exactly balances the weight, and the sphere stops accelerating — it moves at constant "terminal" velocity.

Stokes' law (F=6πηrvF = 6\pi\eta rv) applies only for laminar flow (low Reynolds number, Re < 1). For larger speeds or larger objects, the flow becomes turbulent and the drag force is proportional to v2v^2 instead.

Key proportionality: vtr2v_t \propto r^2. Doubling the radius increases terminal velocity 4 times. This explains why large raindrops fall faster than small ones, and why fine dust particles stay suspended for hours.


Alternative Method

You can use dimensional analysis to verify the formula: [vt]=[r2][ρ][g]/[η]=m2×kg/m3×m/s2/(Pa⋅s)=m/s[v_t] = [r^2][\rho][g]/[\eta] = \text{m}^2 \times \text{kg/m}^3 \times \text{m/s}^2 / (\text{Pa·s}) = \text{m/s}. The numerical coefficient (2/9) must come from the actual derivation.

💡 Expert Tip

For NEET, remember these proportionalities: vtr2v_t \propto r^2, vt(ρsρf)v_t \propto (\rho_s - \rho_f), vt1/ηv_t \propto 1/\eta. MCQs often ask "if radius is doubled, what happens to terminal velocity?" Answer: it becomes 4 times. No calculation needed.


Common Mistake

⚠️ Common Mistake

Students often use ρs\rho_s instead of (ρsρf)(\rho_s - \rho_f) in the formula, forgetting the buoyancy correction. Without buoyancy, the terminal velocity is overestimated. The buoyant force is significant — in this problem, ρf=1300\rho_f = 1300 kg/m³ is about 16% of ρs\rho_s. Always subtract the fluid density from the sphere density.

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