Lesson 11: Fluids

Week 11 — Liquids, gases, and the forces between them

🎯 Learning Objectives

🎯 Intuition First: Why Do Ships Float?

Imagine a steel block in water. It sinks. But a steel ship — which is mostly empty space — floats. Why? Because what matters isn't the material, but the average density of the whole object compared to the fluid. A ship displaces a volume of water whose weight equals the ship's weight.

💡 Key Question:

Why does water pressure increase as you dive deeper? Because you're supporting the weight of all the water above you. The deeper you go, the more water is stacking on top.

📋 Pressure

Pressure: P = F/A
Units: Pascal (Pa) = N/m²
Hydrostatic pressure at depth h: P = ρgh + P₀

Atmospheric pressure: Patm = 1.013 × 10⁵ Pa = 1 atm = 760 mmHg

📝 Pascal's Principle:

Pressure applied to an enclosed fluid is transmitted equally in all directions. This is the basis of hydraulic lifts!

P₁ = P₂   →   F₁/A₁ = F₂/A₂

📋 Buoyancy (Archimedes' Principle)

Fb = ρfluid × Vdisplaced × g

The upward buoyant force equals the weight of the fluid displaced by the object.

📝 Worked Example: Floating Object

A block of wood (density 600 kg/m³, volume 0.02 m³) floats in water (density 1000 kg/m³). What fraction of the block is submerged?

Step 1 — Weight of block:

W = ρwoodVg = 600 × 0.02 × 9.8 = 117.6 N

Step 2 — Buoyant force = weight (floating):

ρwaterVsubg = 117.6 N
Vsub = 117.6/(1000 × 9.8) = 0.012 m³

Step 3 — Fraction submerged:

f = Vsub/V = 0.012/0.02 = 0.6 = 60%

✅ 60% of the block is underwater. (In general, f = ρobjectfluid)

📋 Bernoulli's Equation

P + ½ρv² + ρgh = constant (along a streamline)

This expresses energy conservation for flowing fluids: pressure + kinetic energy density + potential energy density = constant.

💡 Intuition:

Where a fluid flows faster, the pressure is lower. This is why airplane wings generate lift, why a shower curtain gets sucked inward, and why perfume sprays work!

📝 Worked Example: Water in a Pipe

Water flows through a pipe that narrows from 10 cm² to 4 cm². In the wide section, speed is 2 m/s. Find the speed and pressure difference in the narrow section. (Assume horizontal pipe, ρ = 1000 kg/m³)

Step 1 — Continuity equation (Av = constant):

A₁v₁ = A₂v₂
(10)(2) = (4)v₂
v₂ = 20/4 = 5 m/s

Step 2 — Bernoulli (horizontal: h₁ = h₂):

P₁ + ½ρv₁² = P₂ + ½ρv₂²
P₁ − P₂ = ½ρ(v₂² − v₁²) = ½(1000)(25 − 4)
P₁ − P₂ = 500 × 21 = 10,500 Pa

✅ v₂ = 5 m/s, pressure drops by 10,500 Pa in the narrow section

📋 Equation of Continuity

A₁v₁ = A₂v₂ (for incompressible fluids)

What goes in must come out. If the pipe narrows, the fluid must speed up.

✏️ Practice Problems

Problem 1: A hydraulic lift has a small piston (area 5 cm²) and a large piston (area 50 cm²). If 100 N is applied to the small piston, what force does the large piston exert?

Problem 2: An object with density 800 kg/m³ is placed in water. Will it float or sink?

Problem 3: Water flows at 3 m/s in a pipe of area 6 cm², then enters a pipe of area 2 cm². What is the new speed?

✅ Check Your Understanding

Q1: Why is it harder to swim in deep water?

Click to reveal answer

Pressure is higher at depth. At greater depths, the water pressure is higher (P = ρgh), so your body feels more compressed. Also, waves are more powerful deeper out.

Q2 (mini-problem): A 2-kg block (density 4000 kg/m³) is submerged in water. What is the buoyant force?

Click to reveal answer
V = m/ρ = 2/4000 = 0.0005 m³
Fb = ρwaterVg = 1000 × 0.0005 × 9.8 = 4.9 N

Answer: 4.9 N (apparent weight = 2(9.8) − 4.9 = 14.7 N)