Inputs

This page uses the ideal point-mass circular-orbit model. Atmospheric drag, J₂, third-body gravity, ephemerides, and finite burns are not included.

Results

Circular orbital velocity

The model uses v = √(μ/r) and T = 2π√(r³/μ), where r is measured from the central-body center, not from the surface.

Planning boundary

Use the full Orbital Mechanics Workbench or Orbital Mechanics Simulator when eccentricity, maneuvers, perturbations, transfer geometry, or trajectory propagation matter.

Engineering reference

Orbital Velocity Calculator: background and worked detail

Use the Orbital Velocity Calculator to calculate circular orbital speed, period, local gravity, angular rate, specific orbital energy, and angular momentum from altitude around a selected central body.

Shared workbench engineReviewed August 10, 2026Calculation methodology

Circular orbital velocity from first principles

A circular orbit balances inward gravitational acceleration with centripetal acceleration. The entered altitude is converted to orbital radius by adding the central body's reference radius; orbital velocity then follows from the body's gravitational parameter μ.

The result is an ideal two-body circular-orbit state. Atmospheric drag, oblateness, third-body gravity, thrust, inclination, eccentricity, rotating reference frames, and navigation frames are outside this focused calculation.

Equations used by this calculator

Circular speed

v = √(μ/r)

Circular speed depends on the central body's gravitational parameter and distance from its center.

Orbital period

T = 2π√(r³/μ)

Kepler's third-law form gives the circular orbit period.

Specific orbital energy

ε = −μ/(2r)

Bound circular orbits have negative specific mechanical energy.

Worked example

400 km circular Earth orbit

Select Earth and enter 400 km altitude.

  1. Earth radius is added to the 400 km altitude to obtain orbital radius.
  2. Circular speed is about 7.67 km/s.
  3. The period is about 92.6 minutes.

Result: Local gravitational acceleration is about 8.68 m/s², showing that low-Earth-orbit weightlessness is caused by free fall rather than negligible gravity.

Validation checks

Known reference orbits give these checks an unambiguous expected value.

Higher orbit

Case: Increase altitude while keeping the central body fixed.

Expected: Circular speed should decrease while orbital period increases.

Surface-radius limit

Case: Compare 0 km altitude with a small positive altitude.

Expected: The small altitude increase should slightly reduce speed and gravity, with no discontinuity.

Two-body assumptions

Assumptions

  • A point-mass two-body gravitational model.
  • The selected body's gravitational parameter and reference radius are treated as constants.
  • The orbit is circular at the entered radius.

Limitations

  • Does not include atmospheric drag or body oblateness such as J2.
  • Not a trajectory propagator or launch, rendezvous, station-keeping, or reentry model.

Orbital Velocity Calculator FAQ

Why is gravity still high in low Earth orbit?

Gravity at a few hundred kilometres altitude remains a large fraction of surface gravity. Orbiting objects feel weightless because they and their spacecraft are continuously falling together.

Do I enter altitude or distance from Earth's center?

Enter altitude above the selected body's reference surface. The calculator adds the body's radius internally.

Can this calculate an elliptical orbit?

This focused route is for circular orbits. The full Orbital Mechanics Workbench includes elliptical-orbit and additional maneuver analysis.

Where this calculation comes from

Shared with the Orbital Mechanics Workbench, which handles elliptical orbits, perturbations, and transfer planning.