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FLD-24

Archimedes buoyancy

F = ρ g V. The buoyant force equals the weight of displaced fluid.

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FluidsArchimedes

Governing equation

Fb=ρgVF_b=\rho g V

where

\rho
Fluid density (kg/m³)
V
Displaced volume (L)
F_b
Buoyancy (N)

Lecture brief

Historical brief

Bernoulli, Navier–Stokes, Reynolds (1883) and Stokes drag made continuum flow a dimensionless craft. The sheets compute head, drag, Re and a pedagogical NS snapshot. This sheet (FLD-24 — Archimedes buoyancy) is the form associated with Archimedes. Working symbols: ρ\rho, VV \rightarrow FbF_b. Surface integral of hydrostatic pressure. A floating body displaces its own weight.

Purpose

Purpose: compute FbF_b from ρ\rho, VV in Fluid physics via Fb=ρgVF_b=\rho g V F = ρ g V. The buoyant force equals the weight of displaced fluid. Use it when a real fluid physics question must be answered in SI before a code check.

Live realistic example

In symbols

Live case. Given ρ=1000.000kg/m3\rho = 1000.000\,\mathrm{kg/m^{3}}, V=40.000LV = 40.000\,\mathrm{L}, the governing relation Fb=ρgVF_b=\rho g V yields Fb=392.4NF_b = 392.4\,\mathrm{N}. A submerged block, an upward arrow. Move a slider: the numbers are this situation, not a canned story.

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Inputs

Outputs

  • Buoyancy F_b392.4 N
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FLD-24 · pipe
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Narration of this film

A submerged block, an upward arrow.

Surface integral of hydrostatic pressure. A floating body displaces its own weight.

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Watch on YouTube