Explore rotation effects with the Rossby number. Choose units, compute Coriolis from latitude, and compare. Understand when geostrophic balance breaks in real flows today.
The Rossby number compares inertial acceleration to Coriolis effects: Ro = U / (|f| L). When latitude is used, the Coriolis parameter is computed as f = 2Ω sin(φ).
The Rossby number is a dimensionless ratio that compares inertial motion to rotational influence. It is defined as Ro = U / (|f| L), where U is a characteristic speed, L is a characteristic length scale, and f is the Coriolis parameter. Smaller values indicate stronger rotational control.
In large-scale weather systems and ocean currents, rotation can dominate force balances. When Ro is small, pressure-gradient forces often balance Coriolis acceleration, producing near-geostrophic flow. This is why synoptic storms, jet streams, and major ocean gyres show organized, slowly evolving structures at planetary scales.
A practical guideline is: Ro < 0.1 suggests rotation-dominated dynamics; 0.1–1 indicates mixed behavior; and Ro > 1 implies inertia is comparable or stronger. For example, many mid-latitude synoptic systems fall near Ro ≈ 0.1, while small vortices often exceed 10.
Select U to match the phenomenon and the scale L. For storms, use typical wind speed at the relevant altitude. For ocean eddies, use surface or depth-averaged current speed. For rotating machinery flows, use tangential or bulk velocity where rotation-driven effects are evaluated.
The length scale should represent the dominant spatial variation of the flow, such as storm radius, eddy diameter, or channel width. Using L that is too small can inflate Ro and understate rotation, while choosing L too large can overstate rotational control. Consistency with U is key.
When using latitude, this calculator computes f = 2Ω sin(φ). For Earth, Ω ≈ 7.292×10⁻⁵ rad/s. At 45°, this yields |f| ≈ 1.03×10⁻⁴ s⁻¹. Near the equator, sin(φ) approaches zero, making f small and Ro large for the same U and L.
Try U=10 m/s, L=1000 km, φ=45°: Ro ≈ 0.10, typical of large weather systems. For a small lab vortex with U=0.5 m/s and L=0.2 m, the result is often Ro in the tens of thousands, showing negligible Coriolis influence.
Avoid mixing scales, such as a local gust speed with a continental length scale. Remember the calculator uses |f| in Ro, so hemisphere affects sign of f but not the magnitude of rotational influence. When results seem extreme, revisit units, choose consistent scales, and compare with the advective and rotational timescales shown above.
Yes. Because it is a ratio of terms with matching units, Ro has no units. This makes it useful for comparing different flows, locations, and systems on a common scale.
The magnitude of Coriolis influence depends on |f|. The sign of f indicates hemisphere and rotation direction, but the relative strength in Ro is set by its absolute value.
Near φ=0°, sin(φ) is small, so f approaches zero. That often produces large Ro, meaning rotation has weaker control at the same speed and length scale.
Use a scale tied to the dominant circulation, often the radius of maximum winds or the storm-core radius. If you are studying the entire synoptic system, use a larger radius aligned with the broader pressure pattern.
Yes. Select the option to enter f and provide its value in s⁻¹ (or min⁻¹). This is useful for idealized models, lab experiments, or when f is known from a reference.
Values near one indicate inertia and rotation are comparable. Expect stronger curvature, ageostrophic accelerations, and time-dependent behavior than in low-Rossby flows, while still seeing some rotational organization depending on the setting.
Not always. Small Ro supports geostrophic balance, but stratification, friction, boundaries, and strong time dependence can introduce deviations. Use Ro as a first check, then consider context.
| Scenario | U (m/s) | L (m) | Latitude (°) | f (s⁻¹) | Ro | Typical behavior |
|---|---|---|---|---|---|---|
| Synoptic weather system | 10 | 1,000,000 | 45 | ≈1.03×10⁻⁴ | ≈0.10 | Rotation strongly shapes large-scale flow |
| Mesoscale convective feature | 15 | 100,000 | 30 | ≈7.29×10⁻⁵ | ≈2.06 | Ageostrophic effects become important |
| Small lab vortex | 0.5 | 0.2 | 45 | ≈1.03×10⁻⁴ | ≈24,000 | Inertia dominates; rotation is negligible |
Important Note: All the Calculators listed in this site are for educational purpose only and we do not guarentee the accuracy of results. Please do consult with other sources as well.