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.
Referenced by
equation
machine
skill
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