Fluid mechanics begins with understanding the fundamental properties of fluids: density and pressure. These concepts form the foundation for analyzing fluid behavior in both static and dynamic situations.
Density
Density is mass per unit volume, measuring how tightly matter is packed:
ρ=Vm
📚 Practice Problems
1Problem 1easy
❓ Question:
A cube of aluminum has sides of length 5.0 cm. The density of aluminum is 2700 kg/m³. What is the mass of the cube?
Fluid density, pressure, Pascal's principle, and pressure variation with depth
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Start by reading the study notes and working through the examples on this page. Then use the flashcards to test your recall. Practice with the 8 problems provided, checking solutions as you go. Regular review and active practice are key to retention.
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Density and Pressure is part of the AP Physics 2 course on Study Mondo, specifically in the Fluid Mechanics section. You can explore the full course for more related topics and practice resources.
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where:
ρ (rho) = density (kg/m³)
m = mass (kg)
V = volume (m³)
Common Densities:
Material
Density (kg/m³)
Water
1000
Ice
917
Air (STP)
1.29
Mercury
13,600
Aluminum
2700
Gold
19,300
Specific Gravity
Specific Gravity (SG) is the ratio of a substance's density to water's density:
SG=ρwaterρsubstance
Dimensionless (no units)
SG < 1: floats in water
SG > 1: sinks in water
Pressure
Pressure is force per unit area:
P=AF
where:
P = pressure (Pa or N/m²)
F = force perpendicular to surface (N)
A = area (m²)
Common Units:
Pascal (Pa): 1 Pa = 1 N/m²
Atmosphere (atm): 1 atm = 101,325 Pa ≈ 101 kPa
Bar: 1 bar = 100,000 Pa
mmHg: 760 mmHg = 1 atm
psi: 14.7 psi = 1 atm
Pressure in Fluids
Unlike solids, fluids cannot sustain shear stress - they flow. This creates unique pressure properties:
Pressure acts perpendicular to surfaces - fluid pressure always pushes normal to any surface
Pressure is isotropic - equal in all directions at a point
Pressure increases with depth
Pressure vs. Depth
For a fluid at rest, pressure increases linearly with depth:
P=P0+ρgh
where:
P = pressure at depth h
P0 = pressure at surface (usually atmospheric)
ρ = fluid density (kg/m³)
g = 9.8 m/s²
h = depth below surface (m)
💡 Key Insight: Pressure depends only on vertical depth, not container shape!
Gauge vs. Absolute Pressure
Absolute pressure: Total pressure including atmosphere
Pabsolute=Patm+Pgauge
Gauge pressure: Pressure relative to atmosphere
Pgauge=ρgh
Most pressure gauges (like tire gauges) read gauge pressure.
Pascal's Principle
Pascal's Principle: A change in pressure applied to an enclosed fluid is transmitted undiminished to every point in the fluid.
Small piston moves far, large piston moves little distance.
Atmospheric Pressure
At sea level:
Patm=101,325 Pa=101.3 kPa=1 atm
This is equivalent to:
10.3 m column of water
760 mm column of mercury
Atmospheric pressure decreases with altitude.
Problem-Solving Strategy
Identify pressure type needed (gauge or absolute)
Choose reference point (usually surface)
Apply P=P0+ρgh
Remember h is vertical depth only
Check units (convert to SI)
Common Mistakes
❌ Forgetting atmospheric pressure in absolute calculations
❌ Using horizontal distance for h
❌ Mixing gauge and absolute pressure
❌ Unit confusion (1 atm ≠ 1 Pa)
❌ Thinking pressure depends on container shape
=0.050
Density: ρAl=2700 kg/m³
Find: Mass m
Solution:
Step 1: Calculate volume of cube.
V=L3=(0.050)3=1.25×10−4 m3
Step 2: Use density formula.
m=ρV=(2700)(1.25×10−4)=0.338 kg
Answer:338 g
2Problem 2easy
❓ Question:
A cube of aluminum has sides of length 5.0 cm. The density of aluminum is 2700 kg/m³. What is the mass of the cube?
💡 Show Solution
Given:
Side length: L=5.0 cm =0.050 m
Density: ρAl=2700 kg/m³
Find: Mass m
Solution:
Step 1: Calculate volume of cube.
V=L3=(0.050)3=1.25×1
Step 2: Use density formula.
m=ρV=(2700)(1.25×10−4)=0.338 kg
Answer:338 g
3Problem 3medium
❓ Question:
A submarine is at a depth of 200 m below the ocean surface. The density of seawater is 1025 kg/m³. What is the absolute pressure at this depth? What is the gauge pressure?
Step 3: Convert to atmospheres.
Pabsolute=1.01×10
Answer:
Gauge: 2.01 MPa
Absolute: 2.11 MPa or 20.9 atm
4Problem 4medium
❓ Question:
A submarine is at a depth of 200 m below the ocean surface. The density of seawater is 1025 kg/m³. What is the absolute pressure at this depth? What is the gauge pressure?
Step 3: Convert to atmospheres.
Pabsolute=1.01×10
Answer:
Gauge: 2.01 MPa
Absolute: 2.11 MPa or 20.9 atm
5Problem 5medium
❓ Question:
A cube of metal with sides of 5.0 cm has a mass of 1.5 kg. (a) What is its density? (b) Will it float in water (ρ_water = 1000 kg/m³)? (c) What is the pressure at the bottom of the cube when it rests on a table?
(b) Will it float?
ρ_metal = 12,000 kg/m³ > ρ_water = 1000 kg/m³
No, it will sink (denser than water)
(c) Pressure at bottom:
Weight: W = mg = 1.5 × 10 = 15 N
Area: A = (0.050)² = 2.5 × 10⁻³ m²
P = F/A = 15/(2.5 × 10⁻³) = 6,000 Pa or 6.0 kPa
6Problem 6hard
❓ Question:
A hydraulic lift has an input piston (diameter 5.0 cm) and output piston (diameter 30 cm). (a) What force must be applied to lift a 2000 kg car? (b) If the input piston is pushed down 20 cm, how far does the car rise?
💡 Show Solution
Given:
d1=5.0 cm =0.050 m, d2=30 cm =0.30 m
Car mass: m=2000 kg
Solution:
Part (a): Find input force
Step 1: Calculate areas.
A1=πr12=
Step 2: Find output force (car weight).
F2=mg=(2000)(9.8)=19,600 N
Step 3: Apply Pascal's principle.
F1=F2
Part (b): Find output displacement
Step 4: Use volume conservation.
A1d1=A2d
Answer:
(a) Input force: 543 N
(b) Car rises: 5.5 mm
Mechanical advantage = 36, but distance disadvantage = 36. Energy conserved!
7Problem 7hard
❓ Question:
A swimming pool is 2.5 m deep. (a) What is the absolute pressure at the bottom? (b) What is the gauge pressure at the bottom? (c) What is the force on a 2.0 m × 1.0 m rectangular section at the bottom? Use ρ_water = 1000 kg/m³, P_atm = 1.01 × 10⁵ Pa, g = 10 m/s².
💡 Show Solution
Solution:
Given: h = 2.5 m, ρ = 1000 kg/m³, P_atm = 1.01 × 10⁵ Pa
(a) Absolute pressure:
P = P_atm + ρgh
P = 1.01 × 10⁵ + (1000)(10)(2.5)
P = 1.01 × 10⁵ + 2.5 × 10⁴
P = 1.26 × 10⁵ Pa or 126 kPa
(b) Gauge pressure:
P_gauge = ρgh = (1000)(10)(2.5) = 2.5 × 10⁴ Pa or 25 kPa
(c) Force on bottom:
Area = 2.0 × 1.0 = 2.0 m²
F = PA = (1.26 × 10⁵)(2.0)
F = 2.52 × 10⁵ N or 252 kN
Note: If using gauge pressure, F = (2.5 × 10⁴)(2.0) = 5.0 × 10⁴ N (force due to water only)
8Problem 8hard
❓ Question:
A hydraulic lift has an input piston (diameter 5.0 cm) and output piston (diameter 30 cm). (a) What force must be applied to lift a 2000 kg car? (b) If the input piston is pushed down 20 cm, how far does the car rise?
💡 Show Solution
Given:
d1=5.0 cm =0.050 m, d2=30 cm =0.30 m
Car mass: m=2000 kg
Solution:
Part (a): Find input force
Step 1: Calculate areas.
A1=πr12=
Step 2: Find output force (car weight).
F2=mg=(2000)(9.8)=19,600 N
Step 3: Apply Pascal's principle.
F1=F2
Part (b): Find output displacement
Step 4: Use volume conservation.
A1d1=A2d
Answer:
(a) Input force: 543 N
(b) Car rises: 5.5 mm
Mechanical advantage = 36, but distance disadvantage = 36. Energy conserved!
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Yes, this page includes 8 practice problems with detailed solutions. Each problem includes a step-by-step explanation to help you understand the approach.