A metallic sphere of sp.gr. 8.0 falls in an oil of density 800 kg/m³. The diameter of the sphere is 10mm and it attains a terminal velocity of 50mm/s. Find the viscosity of the oil in Poise.

Fluid Mechanics Problem Solution

Problem Statement

A metallic sphere of sp.gr. 8.0 falls in an oil of density 800 kg/m³. The diameter of the sphere is 10mm and it attains a terminal velocity of 50mm/s. Find the viscosity of the oil in Poise.

Given Data

Specific gravity of sphere 8.0
Density of sphere (ρs) 8 × 1000 = 8000 kg/m³
Density of oil (ρo) 800 kg/m³
Diameter of sphere (D) 10 mm = 0.01 m
Terminal velocity (V) 50 mm/s = 0.05 m/s
Acceleration due to gravity (g) 9.81 m/s²

Solution Approach

When a sphere falls through a viscous fluid and reaches terminal velocity, three forces are in equilibrium:

  • Weight of the sphere (downward)
  • Buoyant force (upward)
  • Drag force due to viscosity (upward)

For a sphere moving slowly through a viscous fluid, we can apply Stokes’ law to find the viscosity of the oil.

Calculations

Force Balance Analysis

Step 1: At terminal velocity, the weight of the sphere equals the sum of buoyant force and drag force:

Weight of sphere = Buoyant force + Drag force
ρs × g × (1/6)πD³ = ρo × g × (1/6)πD³ + 3πμDV

Where μ is the dynamic viscosity of the oil, and the drag force is given by Stokes’ law: FD = 3πμDV.

Step 2: Substituting the given values:

8000 × 9.81 × (1/6)π × (0.01)³ = 800 × 9.81 × (1/6)π × (0.01)³ + 3π × μ × 0.01 × 0.05

Step 3: Simplifying:

(8000 – 800) × 9.81 × (1/6)π × (0.01)³ = 3π × μ × 0.01 × 0.05
7200 × 9.81 × (1/6)π × 10⁻⁶ = 3π × μ × 0.01 × 0.05
7200 × 9.81 × π × 10⁻⁶/6 = 3π × μ × 0.0005

Step 4: Solving for μ:

μ = (7200 × 9.81 × π × 10⁻⁶/6) ÷ (3π × 0.0005)
μ = (7200 × 9.81 × 10⁻⁶) ÷ (3 × 6 × 0.0005)
μ = (7200 × 9.81 × 10⁻⁶) ÷ (0.009)
μ = 7.848 Pa·s

Step 5: Converting to Poise (1 Pa·s = 10 Poise):

μ = 7.848 Pa·s × 10 = 78.48 Poise

Step 6: Verifying that Reynolds number is less than 0.2 for Stokes’ law validity:

Re = ρoVD/μ = (800 × 0.05 × 0.01) ÷ 7.848 = 0.05

Since Re = 0.05 < 0.2, Stokes' law is valid for this problem.

Viscosity of the oil = 78.48 Poise

Detailed Explanation

Terminal Velocity Principle

When an object falls through a fluid, it eventually reaches a constant velocity called terminal velocity. At this point, the downward gravitational force is exactly balanced by the upward forces (buoyancy and drag).

Stokes’ Law

Stokes’ law describes the drag force exerted on spherical objects moving through a viscous fluid:

FD = 3πμDV

Where:

  • μ is the dynamic viscosity of the fluid
  • D is the diameter of the sphere
  • V is the velocity of the sphere relative to the fluid

This law applies when the Reynolds number is less than 0.2, which indicates laminar flow conditions.

Force Analysis

The three forces acting on the falling sphere are:

  1. Weight force: FW = ρs × g × Volume = ρs × g × (1/6)πD³
  2. Buoyant force: FB = ρo × g × Volume = ρo × g × (1/6)πD³
  3. Drag force: FD = 3πμDV

Units Conversion

The viscosity calculated in SI units is 7.848 Pa·s (or N·s/m²). The unit Poise is a CGS unit of dynamic viscosity:

  • 1 Poise = 0.1 Pa·s
  • Therefore, 7.848 Pa·s = 78.48 Poise

Applications

This method of determining fluid viscosity is the principle behind the falling ball viscometer, which is used in various industries:

  • Oil and petroleum industry for quality control
  • Food processing for consistency measurement
  • Pharmaceutical industry for medication viscosity testing
  • Chemical industry for product development and quality assurance

Importance of Reynolds Number

The Reynolds number (Re = 0.05) being well below 0.2 confirms that we are in the creeping flow regime where Stokes’ law applies. This is characterized by:

  • Dominant viscous forces over inertial forces
  • Streamline, laminar flow around the sphere
  • Negligible wake formation behind the sphere

Understanding fluid viscosity is essential in many engineering applications, including lubrication systems, hydraulic machinery, and fluid transport systems.

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