QCC Notes
CLASS 11 · PHYSICSJEE MAIN × NEETहिंदी
§ 9.4NCERT Class 11 · Physics · Chapter 9

Viscosity, Stokes' Law, Terminal Velocity & Poiseuille Flow

Just as solid surfaces in contact experience mechanical friction opposing relative sliding, adjacent layers of a real fluid experience an internal friction opposing relative motion. This internal property of fluids is termed viscosity. Viscous forces dissipate kinetic energy into heat as fluids flow through pipes or past solid obstacles.

1. Velocity Gradient & Newton's Law of Viscosity

Consider a liquid flowing laminar-style over a horizontal fixed solid plate. The layer in direct contact with the solid boundary is stationary (v = 0, the "no-slip" condition). As perpendicular distance x from the fixed plate increases, layer velocity increases continuously up to v:

   Top Layer:      ~~~~~~~~~~~~~~~~==================> Velocity (v + dv)
                   |  Shear Stress tau = F / A       |
                   |  Velocity Gradient = dv / dx    |
   Intermediate:   ~~~~~~~~~~~~~~~~============>       Velocity v
                   |                                 |
   Bottom Plate:   =================================== Fixed Solid Wall (v = 0)
      
Fig 9.4A: Velocity profile in laminar fluid flow showing shear stress generated across adjacent fluid layers.

The rate of change of flow velocity with perpendicular distance is called the velocity gradient (dv/dx), measured in s-1.

According to Sir Isaac Newton, the backward tangential viscous drag force F acting between two adjacent fluid layers of contact area A is:

F ∝ A and F ∝ dv/dx ⇒ F = -η A dv/dx

where η is the coefficient of viscosity of the fluid. The negative sign signifies that viscous drag opposes relative fluid motion.

Units and Dimensions of Viscosity

  • SI Unit: N·s/m2 = Pa·s (also called Decapoise or Poiseuille, Pl).
  • CGS Unit: dyne·s/cm2 = Poise (P).
  • Conversion: 1 Pa·s = 10 Poise = 1000 cP (centipoise). (Water at 20°C has ηw ≈ 10-3 Pa·s = 1 cP).
  • Dimensional Formula: [η] = [M1 L-1 T-1].

2. Stokes' Law & Terminal Velocity Derivation

Stokes' Law: When a small spherical body of radius r moves with velocity v through an infinite, homogeneous, stationary viscous fluid of viscosity η, the retarding viscous force Fv opposing its motion is:
Fv = 6π η r v

Derivation of Terminal Velocity (vt)

Consider a small sphere of radius r and solid density ρ falling vertically under gravity through a viscous medium of density σ (ρ > σ):

                               +-------------------+
                               |   Upward Forces:  |
                               |   FB (Buoyancy)  |
                               |   Fv (Viscous)   |
                               +------------------+
                                         |
                                      ( O ) Sphere (Radius r, Density rho)
                                         |
                               +---------v---------+
                               |  Downward Force:  |
                               |  W = mg (Gravity) |
                               +-------------------+
             
             At Terminal Velocity: W = FB + Fv (Net Acceleration a = 0)
      
Fig 9.4B: Free-body diagram of a spherical ball at terminal velocity in a viscous fluid column.

Three concurrent forces act on the descending sphere:

  1. Downward Gravitational Weight: W = mg = 4/3π r3 ρ g.
  2. Upward Buoyant Upthrust: FB = 4/3π r3 σ g.
  3. Upward Stokes' Viscous Drag: Fv = 6π η r v.

Net downward equation of motion: m a = W - FB - Fv.

As the velocity increases, Fv increases proportionally until the net force becomes zero (a = 0). Thereafter, the sphere falls with a constant maximum steady speed termed terminal velocity (vt):

W = FB + Fv ⇒ 4/3π r3 ρ g = 4/3π r3 σ g + 6π η r vt
6π η r vt = 4/3π r3 (ρ - σ) g
Terminal Velocity Formula:
vt = 2/9(r2(ρ - σ)g)/(η)
Key Proportionalities:
  • vt ∝ r2 (Larger raindrops fall significantly faster than tiny fog droplets).
  • vt ∝ (ρ - σ)(If ρ < σ, such as an air bubble in water, vt is negative, meaning the bubble accelerates upward).
  • vt ∝ 1/(η) (Thicker, more viscous fluids severely reduce terminal velocity).

3. Poiseuille's Law of Capillary Flow

For steady, streamline laminar flow of a viscous liquid through a horizontal cylindrical capillary pipe of radius r and length l under a driving hydrostatic pressure difference P:

Q = dV/dt = (π P r4)/(8 η l)
  • Enormous Fourth-Power Sensitivity (Q ∝ r4): If a capillary tube's radius is halved (r → r/2) while keeping driving pressure constant, the discharge rate drops by a staggering factor of 24 = 16! This is of monumental clinical importance in vascular hemodynamics: minor arterial plaque buildup severely impairs blood flow.
  • Fluid Resistance Analogy: Analogous to Ohm's Electrical Law (I = V / R):
    Q = P/Rfluid where Rfluid = (8η l)/(π r4)

4. Critical Velocity & Reynolds Number

The transition from smooth laminar flow to turbulent, vortex-shedding chaotic flow is governed by the dimensionless Reynolds Number (Re), introduced by Osborne Reynolds:

Re = (Inertial Force)/(Viscous Force) = (ρ v d)/(η)

where ρ is fluid density,vis flow speed,dis pipe diameter, andη is viscosity.

Reynolds Number Range Flow Regime Physical Characteristics
Re < 2000 Laminar (Streamline) Fluid flows in smooth, orderly parallel cylindrical sheets; minimal mixing; quiet.
2000 < Re < 3000 Transitional (Unstable) Flow fluctuates intermittently between laminar streaks and turbulent bursts.
Re > 3000 Turbulent Chaotic, swirling eddies and vortices; high flow resistance and energy dissipation; noisy.

JEE & NEET Solved Practice Problems

Problem 1: Eight identical spherical raindrops, each falling through air with a terminal velocity of 0.1 m/s, coalesce into a single larger spherical raindrop. Assuming air resistance satisfies Stokes' law, determine the terminal velocity of the single combined drop.
Solution:
Let r be the radius of each small drop and R be the radius of the coalesced drop.
By conservation of water volume:
4/3π R3 = 8 × (4/3π r3) ⇒ R3 = 8r3 ⇒ R = 2r

From Stokes' terminal velocity equation:
vt ∝ r2

Therefore:
(vt')/vt = (R/r)2 = 22 = 4

vt' = 4 × 0.1 m/s = 0.4 m/s
Problem 2: A small spherical metal ball of radius 1 mm and density 10.5 g/cm3 falls through a tall column of glycerin (density 1.5 g/cm3, η = 0.8 Pa·s). Calculate the terminal velocity acquired by the ball. Take g = 9.8 m/s2.
Solution:
Converting all quantities to SI units:
- r = 1 mm = 10-3 m
- ρ = 10.5 × 103 kg/m3
- σ = 1.5 × 103 kg/m3 ⇒ ρ - σ = 9.0 × 103 kg/m3
- η = 0.8 Pa·s, g = 9.8 m/s2

Applying the terminal velocity formula:
vt = 2/9(r2(ρ - σ)g)/(η) = 2/9 × ((10-3)2 × (9.0 × 103) × 9.8)/0.8

vt = 2/9 × (10-6 × 9000 × 9.8)/0.8 = 2/9 × 0.0882/0.8 = (2 × 0.0882)/7.2 = 0.1764/7.2 = 0.0245 m/s = 2.45 cm/s

Frequently Asked Questions

Q1. What is the effect of temperature on the viscosity of liquids versus gases?
For liquids, viscosity decreases rapidly as temperature rises because thermal agitation increases intermolecular separation, weakening cohesive forces. For gases, viscosity increases with temperature (proportional to sqrt(T)) because gas viscosity arises from momentum transfer during molecular collisions, which accelerate at higher thermal velocities.
Q2. What is Terminal Velocity, and how does it depend on the radius of a spherical body?
Terminal velocity (vt) is the maximum constant velocity achieved by a falling body in a viscous fluid when the downward gravitational weight is exactly balanced by the sum of upward buoyant upthrust and Stokes' viscous drag. By formula, vt = (2/9) * r2 * (rho - sigma) * g / eta, meaning terminal velocity is directly proportional to the square of the sphere's radius (vt proportional to r2).
Q3. What is Reynolds Number, and what flow regimes does it delineate?
Reynolds number (Re = rho * v * d / eta) is a dimensionless ratio of inertial forces to viscous forces in a fluid flow. For flow through a pipe: (1) Re < 2000 corresponds to smooth laminar (streamline) flow; (2) 2000 < Re < 3000 corresponds to unstable transitional flow; and (3) Re > 3000 corresponds to fully turbulent, chaotic flow.
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