πͺ Lagrange Points
System Display Simulation| Point | x (rel.) | Stable? |
|---|---|---|
| L1 | β | No |
| L2 | β | No |
| L3 | β | No |
| L4 | +0.500 | Yes * |
| L5 | +0.500 | Yes * |
* Stable when Mβ/Mβ > 24.96
Click the canvas to launch a test particle at that position.
What Are Lagrange Points?
In the restricted three-body problem (two massive bodies + a massless test particle), there are five special positions where the gravitational forces and the centrifugal force in the rotating reference frame exactly balance. These are the Lagrange points L1βL5.
- L1 β between the two bodies; used for solar observation (SOHO, DSCOVR).
- L2 β behind the smaller body; host to James Webb Space Telescope, Gaia, Planck.
- L3 β directly opposite the smaller body (unstable).
- L4 & L5 β 60Β° ahead and behind in the orbit; stable if Mβ/Mβ > 24.96. Home to Trojan asteroids (2000+ in SunβJupiter L4/L5).
Effective Potential
The colour map shows the effective potential in the co-rotating frame: $\Phi_{eff} = -\frac{GM_1}{r_1} - \frac{GM_2}{r_2} - \frac{1}{2}\omega^2\rho^2$. Lagrange points are saddle points (L1βL3) or local maxima (L4βL5) of this surface.
Real-World Applications
Dozens of spacecraft occupy L1 and L2 of the SunβEarth system. The Trojan asteroids co-orbit with Jupiter. NASA is studying L4/L5 of EarthβMoon for future space stations. The concept was first described by Joseph-Louis Lagrange in 1772.