Equations · equation

Moment of Inertia

Mechanics · 1765

Equation
I = Σ m_i r_i² = ∫ r² dm
Field
Mechanics
Symbols
I moment of inertia · m_i a bit of mass at distance r_i from the axis · the sum or integral over the whole body
Year
1765

Significance

The rotational counterpart of mass: how hard a body is to spin up, set not just by how much mass it has but by how far from the axis it sits — hence the square. Euler defined it in 1765. A flywheel puts its mass at the rim for exactly this reason; a figure skater pulls arms in to spin faster; a hollow shaft is nearly as stiff in torsion as a solid one for a fraction of the weight.

Skills

Machines

Required By

Referenced by

equation
machine
skill

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From the Equations database in Notion, last edited 2026-08-18. This page is the row, rendered by the build; nothing on it is written by hand.