Section 1.1: Fluids
This section introduces fluid mechanics, including pressure, density, buoyancy, and fluid flow. We examine how fluids behave under different forces and conditions.
Key Equations & Concepts:
- Density: \( \rho = \frac{m}{V} \)
- Pressure: \( P = \frac{F}{A} \)
- Hydrostatic Pressure: \( P = P_0 + \rho g h \)
- Buoyant Force: \( F_b = \rho_{fluid} V_{displaced} g \)
- Continuity Equation: \( A_1 v_1 = A_2 v_2 \)
- Bernoulli's Equation: \( P + \frac{1}{2}\rho v^2 + \rho g h = \text{constant} \)
Example 1
A 2 kg block is submerged in water. Find the buoyant force acting on it if the displaced volume is 0.002 m³.
\( F_b = \rho_{water} V g = 1000 \cdot 0.002 \cdot 9.8 = 19.6 \text{ N} \)
Example 2
Water flows through a pipe with cross-section 0.05 m² at 2 m/s. The pipe narrows to 0.02 m². Find the flow speed in the narrow section.
Using continuity equation: \( A_1 v_1 = A_2 v_2 \Rightarrow 0.05 \cdot 2 = 0.02 \cdot v_2 \Rightarrow v_2 = 5 \text{ m/s} \)
Practice Problems
- Calculate the pressure at 3 m depth in freshwater.
- A cube of side 0.1 m is submerged in water. Find the buoyant force.
- Water flows through a pipe: area 0.1 m², speed 1 m/s. The pipe narrows to 0.05 m². Find new speed.
- Air exerts 101 kPa at sea level. Find force on 0.2 m² surface.
- A metal block weighs 50 N in air and 30 N in water. Find buoyant force.
- Compute hydrostatic pressure at bottom of a 5 m oil tank (\( \rho = 850 \text{ kg/m³} \)).
- Explain why ships float even if made of steel.
- Velocity of fluid doubles. How does pressure change (Bernoulli)?
- A cylinder of radius 0.1 m, area 0.0314 m², has 200 N force applied. Find pressure.
- Water flows from wide section (0.03 m²) at 3 m/s to narrow (0.01 m²). Find speed.