Buoyancy
A short lesson with diagrams, a worked example, a problem to try, and a quick check. Then quiz yourself on 5 practice questions.
A fluid pushes up on anything in it. Archimedes’ principle: the buoyant force equals the weight of the fluid displaced, FB = ρfluidVsubg. Use the fluid’s density and the submerged volume.
1. Float or sink?
2. Where it comes from
Pressure grows with depth, so the fluid pushes harder on the bottom of an object than on its top. That difference is the buoyant force.
Once an object is fully underwater, going deeper doesn’t change FB: the submerged volume stays the same.
Weighing a rock in water reads less than in air. The scale (or string) supports only mg − FB, the apparent weight. Draw a free-body diagram: FB up, tension up, mg down.
3. Example, then try it
A 10 kg rock with volume 0.0040 m³ hangs from a string, fully underwater. Find the buoyant force and the tension in the string. (g = 10 m/s²)
FB = ρVg = (1000)(0.0040)(10) = 40 N.
Equilibrium: T + FB = mg → T = 100 − 40 = 60 N, its apparent weight.
A wooden block (volume 0.010 m³, density 600 kg/m³) floats in water. What fraction is underwater? How hard must you push down to hold it completely under?
Weight: m = ρV = (600)(0.010) = 6.0 kg, so mg = 60 N.
Floating: FB = 60 N → Vsub = 60 ÷ (1000 × 10) = 0.0060 m³, which is 60% of the block (= 600/1000).
Fully under: FB = (1000)(0.010)(10) = 100 N.
Your push: F + mg = FB → F = 100 − 60 = 40 N down.
Answer: 60% underwater; a 40 N push holds it under.
4. Common mistakes
A steel ball and an aluminum ball have the same volume. Both are held completely underwater. How do the buoyant forces on them compare?
FB = ρfluidVsubg. Same fluid, same submerged volume, so the same buoyant force. The steel ball is heavier, but that changes its weight, not FB.
Ready to practice?
5 questions on Buoyancy, each with a hint and an explanation for every wrong answer.
