OrbitLab The Shape of Gravity

GENERAL RELATIVITY / AN ILLUSTRATION

The shape
of gravity.

Mass changes the geometry.
A drawing of the idea, not a calculated metric.

FIELD IN MOTION
An illustrative lattice curves around the Sun and planets. Physical readings and a text explanation are available in About this model.

The mesh illustrates how mass influences spacetime geometry. Warping and body sizes are exaggerated, and orbital distances and mass differences are compressed. It is not a calculated spacetime metric. Select a body to read its physical mass and surface gravity, and adjust its hypothetical mass.

Illustrated influenceWEAKER STRONGER
LATTICE LINES
243
BODIES
9
EXAGGERATION
1.0×
SELECTED BODYSun
SURFACE GRAVITY

274.2 m/s²

SCHWARZSCHILD RADIUS

2.95 km

STARLIGHT BENT AT THE LIMB

1.75 arcsec

SURFACE CLOCK FALLS BEHIND

66.9 s / year

An exaggerated illustration of geometry. Not a literal fabric or a spacetime metric.

12.5 / 50 years
THE SCIENCE BEHIND THE SCENE

Mass changes
the geometry.

In general relativity, mass and energy influence spacetime geometry. Freely falling objects follow geodesics: the straightest possible paths through that geometry.

Read the picture as an analogy

The spatial lattice is a smooth, bounded deformation towards the bodies. The gravity-well view uses a softened potential-like surface. Neither is a calculated spacetime metric or an embedding of the Solar System's actual geometry. There is no physical mesh, downward pull, or material sheet in space.

Sizes are enlarged, orbital distances use a square-root scale, and mass differences are compressed so planets' effects remain visible beside the Sun. Blue-to-gold colour indicates the strength of the illustrated influence, with no physical units. "Undeformed grid" removes only the drawing's warp; it does not switch gravity off.

What the controls calculate

Each mass slider multiplies that body's reference mass while holding its mean radius fixed. The readings use g = GM/R² and rₛ = 2GM/c². Two more come straight from general relativity: starlight grazing the body's edge is turned through 4GM/c²R, and a clock on its surface runs slow by the factor √(1 − rₛ/R). For the Sun that is 1.75 arcseconds, the bending Eddington's expeditions measured at the 1919 eclipse, and about 67 seconds a year. For Earth the clock difference is about 22 milliseconds a year, small but large enough that GPS satellites must correct for it. Surface gravity assumes an isolated spherical body without rotation. The Schwarzschild radius is a characteristic length: these bodies are much larger than that radius and are not black holes.

Planets follow prescribed Keplerian orbits from fixed J2000 elements. Increasing the Sun's mass increases the displayed orbital rate by its square root. Changes to other planets affect the drawing and their readings, not orbital paths. There is no numerical solution of Einstein's equations, mutual planetary perturbations, or relativistic precession. Elapsed time is illustrative, not a calendar date.

Readings at the currently chosen masses
BodyMass factorGravity (m/s²)rₛ (m)Light bent (″)Clock lag (s/yr)

Planet imagery: Mercury, NASA / JHUAPL / Carnegie (MESSENGER); Venus, NASA / JPL (Mariner 10); Earth, NASA / Apollo 17; Mars, ESA / Rosetta OSIRIS, CC BY-SA 3.0 IGO; Jupiter, NASA / New Horizons; Uranus and Neptune, NASA / JPL (Voyager 2). The Sun and Saturn use schematic shading.

Explore at your own pace.

Focus the scene with Tab, then use:

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All controls work with Tab and the arrow keys. Reduced-motion preferences start the simulation paused and turn off camera orbit.