Hill Sphere Radius Calculator

Hill Sphere Radius Calculator

Estimate the gravitational sphere of influence for planets, moons, dwarf planets, asteroids, and exoplanets using periapsis, eccentricity, and mass ratio.

🪐Real presets
Orbit and mass inputs
Mass of the star, planet, or primary object being orbited.
Mass of the planet, moon, dwarf planet, or small body.
Average orbital distance in kilometers.
The formula uses a(1-e), so eccentric paths shrink the usable Hill radius.
Physical radius in kilometers for the surface comparison.
This calculator reports the chosen fraction as a practical outer moon-orbit scale, not as a guaranteed stability boundary.

Hill sphere estimate

Hill sphere radius 0 km
Stable moon limit 0 selected fraction
Hill / body radius 0x compared with physical radius
Hill / orbital radius 0% compared with semi-major axis a
🔢Formula breakdown

rH = a(1-e) (m / 3M)1/3

The calculator first converts masses and distances to common units, finds periapsis distance a(1-e), applies the cube-root mass term, then compares rH with the body's radius and the original orbital radius.

a(1-e) Periapsis term
m / 3M Mass ratio
cube root Gravity scaling
f rH Stable moon scale
📊Solar system comparison table
Orbiting body Primary Eccentricity Approx rH using a(1-e) rH / body radius
MercurySun0.2056175,000 km72x
VenusSun0.00681,000,000 km165x
EarthSun0.01671,470,000 km231x
MarsSun0.0934982,000 km289x
JupiterSun0.048950,500,000 km722x
SaturnSun0.056561,800,000 km1,025x
NeptuneSun0.0087115,000,000 km4,670x
PlutoSun0.24885,750,000 km4,840x
🛰Stable moon orbit fraction guide
Fraction Use case Interpretation Best for
0.25 rHCompact conservative limitExtra clearance from perturbationsHigh-eccentricity systems
0.33 rHLong-term prograde marginUseful first-pass moon zoneHabitability screens
0.50 rHCommon prograde estimateBroad practical outer scaleSolar system comparisons
0.70 rHRetrograde upper estimateRetrograde orbits can extend fartherDynamical experiments
Mass and distance constants
Quantity Symbol Value used Notes
Solar massM sun1.98847e30 kgDefault stellar mass unit
Earth massM earth5.9722e24 kgPlanet and moon comparisons
Jupiter massM jupiter1.89813e27 kgGas giant and exoplanet inputs
Astronomical unitAU149,597,870.7 kmAverage Earth-Sun distance
Milemi1.609344 kmConverted internally to km
🔍Result interpretation table
Output Calculation What it compares How to read it
Hill sphere radiusa(1-e)(m/3M)^1/3Orbiting body's gravity reachLarger means a wider satellite region
Stable moon limitfraction x rHPractical satellite orbit scaleUse smaller fractions for stricter screens
Hill / body radiusrH divided by radiusGravity reach versus surface sizeLow values leave little clearance
Hill / orbital radiusrH divided by aSphere size versus orbital distanceUsually a small percentage
🧭Practical calculation tips
Use periapsis for eccentric systems. The correct input path is rH = a(1-e)(m/3M)1/3, so ignoring eccentricity can overstate the smallest Hill sphere a body experiences during its orbit.
Compare against the physical radius. A Hill radius that is only a few body radii wide leaves limited room for long-lived satellites, rings, or close spacecraft parking orbits.

When we think about gravitational force of a planet, it’s easy to think of it as basic sphere. Imagine that there’s a transparent bubble and all of the moons and other debris clings to the parent world. In reality, it’s more complicated. Depending on distance of a planet from its primary star; and mass of that star, the gravitational effect vary and so does its shape. The eccentricity of orbit even comes into play here.

What we call the Hill sphere refers to the region around a planet where gravity force of the planet exceed that of the central star. And guess what? That’s not theoretical either; it explains why a planet retain a moon (or doesn’t). It also explains if a satellite will be lost forever in outer space.

Understanding the Hill Sphere

This boundary has easy math. It’s a function off the distance between two bodies and their masses compared to each other. Put in the planet and star mass. Put in orbital semi-major axis. The tool will do the math and spit out a kilometer radius.

But what does that mean? What does that number mean practicaly? That’s where oddness of orbit comes into play. Not all orbits is circular. In fact, most aren’t. The gravity of star exerts more force on planet as it approaches its closest point. The pull of the star shrink the Hill sphere at that moment. Using the average distance may overestimate stability. This means people makes wrong assumptions about whether a satellite could stays in orbit over time.

Determine what portion of the Hill sphere is usable for stable moons. For this, we need fraction that can be used for a stable orbit. According to research, moons will remains stable in roughly half the Hill radius when they are prograde. Prograde means that moon orbits in the same direction as rotation of the planet. When it’s retrograde, it may remain stable until it reaches about 70% of the radius. Using the calculator, you can change this fraction and visualize how this affect the available space. It might not seem like much, but it makes a huge differance. After all, you want your satellite to survive for billions of year. Otherwise, tidal forces will strip the satellite away.

Another way to understand the Hill radius is to compare it to planet’s physical radius. When the Hill sphere is big compared to planet, then we know there is plenty of space to have lots of moons. We will have room for rings and orbital infrastructure too. When ratio is small, then we know it will be a cramped place. Gravitational disturbances can easily pushes satellites out of their orbits.

The table on the page are a reference. You’ll see that Jupiter has a huge sphere which holds its complex moon system. Mercury have a tiny sphere with not much room for any natural satellites. Knowing these ratios helps us explain how some worlds doesn’t have any moons at all. And others has lots of them.

Students can use it. Worldbuilders can use it. Anyone interested in how the solar system work can use it. It’s no longer necessary to memorize constants. You don’t have to fret over mismatched units, e.g., kilograms vs. Solar masses. Just enter the numbers and the gravitational range is revealed.

Why doesn’t Mars have big moons? What would an actualy habitable zone look like on a fictional planet? How could I create a realistic one? Questions like these is answered with context provided by the Hill sphere. It connects the math of orbits to the real-world structures in our solar system.

The Hill sphere is about limits. It marks the end of where a planet’s gravity holds control. And exploring those limits help you understand the balance that maintains order in the solar system. It reveals relationship among time, distance, and mass. It shows why certain worlds holds onto their moons while others drop theirs. With these numbers you can see those bounds, making abstract physics into concrete understanding.

Hill Sphere Radius Calculator