Galileo number#
Named after: Galileo Galilei (1564-1642).
$$\text{Ga} \stackrel{\text{def}}{=} \frac{g L^{3}}{\nu^{2}} \sim \frac{\text{gravity driven motion}}{\text{viscous diffusion}}$$
Description#
Measures gravity-driven motion relative to viscous diffusion. It is useful for settling, rising bubbles, and natural motion set by body forces.
Quantities#
| Name | Symbol | SI units | Dimension |
|---|---|---|---|
| gravitational acceleration | \(g\) | \(\mathrm{m}\,\mathrm{s}^{-2}\) | \(\text L\,\text T^{-2}\) |
| characteristic length | \(L\) | \(\mathrm{m}\) | \(\text L\) |
| kinematic viscosity | \(\nu\) | \(\mathrm{m}^{2}\,\mathrm{s}^{-1}\) | \(\text L^{2}\,\text T^{-1}\) |
Regimes#
Settling and natural motion
| Range | Regime | Description |
|---|---|---|
| 0 – 1 | viscous settling | Viscous resistance controls motion. Falling particles or bubbles move slowly and remain in a creeping flow regime. |
| 1 – 1000 | transitional settling | Gravity driven motion is affected by both viscosity and inertia. Wakes and path instabilities may begin to appear. |
| 1000 – ∞ | inertial settling | Inertial effects dominate gravitational motion. Wakes, vortex shedding, and unsteady trajectories become important. |