FLD-20
Vorticity (rigid rotation)
ω = 2 Ω. For rigid-body rotation the vorticity is twice the angular velocity.
Governing equation
where
- \Omega
- Angular velocity (rad/s)
- \omega
- Vorticity (1/s)
The figure, part by part
Each numbered marker wears the color of its card. Hover a card to light the marker. Tap a marker to jump to that card. The slider walks a red point along the curve; Animate drawing traces it like a pen.
Governing law — red
Domain of the variable — blue
Response curve — green
Rate of change — amber
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-20 — Vorticity (rigid rotation)) is the form associated with Helmholtz. Working symbols: . ω = ∇×v. Kelvin and Helmholtz constrain how vortex lines move in an inviscid barotropic fluid.
Purpose
Live realistic example
In symbols
Calculator
Inputs
Outputs
- Vorticity \omega8.00 1/s
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Free library
Full libraryFree PDF / open book
- University Physics Vol. 1 (mechanics, waves)OpenStax · CC BY · Free PDF / open book
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- LibreTexts PhysicsLibreTexts · CC · Free PDF / open book
- SI Brochure (BIPM)BIPM · Free PDF / open book
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Narration of this film
A spinning cylinder of fluid, a vorticity vector.
ω = ∇×v. Kelvin and Helmholtz constrain how vortex lines move in an inviscid barotropic fluid.
Watch on YouTube