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Science Astronomy Atmosphere

Vol. Science · Astronomy · The speed

Escape
and the orbit

Two speeds belong to one distance from a body’s center. A circular orbit needs v = √(GM/r). Leaving, and never coming back, needs vesc = √(2GM/r). The second is the first times √2. The NASA NSSDCA fact sheets print GM and a volumetric mean radius for the Moon and each planet. This desk uses those two numbers. At altitude 0 on Earth, GM = 0.39860 × 106 km3/s2 and R = 6,371.000 km give 11.186 km/s, the escape velocity the Earth Fact Sheet lists. The Gravity desk names Newton’s cannon and does not compute these speeds. The year of a solar orbit is the Kepler desk. The half-ellipse between two of those circles is the Hohmann desk. Speed anywhere on one ellipse is the vis-viva desk. The neighborhood those orbits sit in is the solar map.

Classroom schematic. The body is a smooth sphere with the volumetric mean radius. The launch is sideways, from rest relative to a body that is not spinning. No air, so no drag. No thrust after the speed is set. The drawing is Newton’s cannon as a diagram: paths are conic sections, clipped when they leave the frame. It is not a launch window, not a trajectory a spacecraft could fly, and not mission-planning data. Miles per hour are a conversion of the computed km/s. They are not a second NASA table.

Interactive · One radius

Sideways launch · body to scale with altitude · no air, no spin

  • Falls back
  • Circular
  • Ellipse
  • Escape
  • Your launch
0 km
—

What this means

Escape speed does not care which way you point, or how heavy the projectile is, in this model. The speed is the one that makes kinetic energy equal the depth of the well: ½mv² = GMm/r, so v = √(2GM/r). The projectile’s mass cancels. Direction never enters the energy. The same speed, aimed any way that stays clear of the sphere, still coasts to infinity. Aim into the sphere and you hit it even above escape speed. The drawing fires sideways, the cannon way. Straight up at the same speed is a different path and the same threshold.

A rocket does not have to be at escape speed in one instant. Escape speed is a coasting speed at one place, with the engine already off. A rocket can thrust for minutes and add energy the whole way. It may never pass through the surface escape speed as a single reading. Most launches are not trying to escape. A circular orbit needs less speed, by exactly √2. The vehicle climbs, turns, and settles into that slower circle. This page has no throttle. The slider is the speed at the moment the coast begins.

Air and rotation are left out on purpose. A spinning body gives an eastward launch a head start. An atmosphere takes speed back as drag, and it makes a surface-grazing circle impossible. The fact-sheet notes define escape velocity as the speed at the surface needed to escape, ignoring atmospheric drag, and for a gas giant that surface is the 1-bar level. This sphere uses the volumetric mean radius, because that is the radius that reproduces the sheet’s mean gravity. Jupiter, Saturn, Uranus, and Neptune list an escape speed that matches the equatorial 1-bar radius instead. Both radii are on the sheet. The readout keeps them apart.

Literacy · two speeds, one radius

Circular orbit
Sideways speed √(GM/r). The path is a circle of that radius. In the drawing it is the dashed gold curve through the launch point. At altitude 0 it lies on the limb: a grazing circle, only because this model has no air and no terrain.
Escape speed
Sideways, or any other direction that clears the sphere, at √(2GM/r). The path is a parabola. Faster than that, the path is a hyperbola. Both leave and do not return. The ratio of escape speed to circular speed is √2 at every altitude. Altitude changes both speeds. It does not change the ratio.
Falls back
The coast intersects the sphere. On the surface, every speed below circular does that. Above the surface, a slow ellipse can still miss the ground. The button marked Falls back picks a speed that hits.
Ellipse
A closed coast that misses the sphere and is not a circle. The button picks 1.2 times circular speed, so the launch point is the near end and the far end may leave the frame. The frame does not shrink to chase it.
Gravity at this radius
GM/r², in m/s². At altitude 0 this is the fact sheet’s mean surface gravity (for a gas giant, gravity at the mean 1-bar radius). It is the pull per unit mass. It is not a reading from a scale on a spinning world.
What the sphere leaves out
Drag, lift, thrust, rotation, equatorial bulge, and density lumps. The Gravity desk already says an orbit is falling sideways. This page is only the two speeds. Gas-giant escape speeds on the fact sheets match √(2GM/Req) at the equatorial 1-bar radius. Mean gravity matches GM/R² at the volumetric mean radius. The presets use the volumetric radius for both readouts, and the cadence says when the sheet’s escape speed is the equatorial one. Custom mass is NIST G times the kilograms you type. It is not a fact-sheet GM.

Sources · public NASA pages

Cited, not invented

Classroom picture of two speeds at one radius. GM and the volumetric mean radius are the fact sheets’ printed figures. Earth’s surface escape on this page is 11.186 km/s because that is what those two figures produce, and it is what the Earth Fact Sheet lists. Not a trajectory, not a launch, and not mission-planning data. Earthrise preview: NASA / Bill Anders (public domain).

Keep going

The pull

Gravity

Newton’s cannon, named. Weight, orbits, and the gap this speed formula does not close.

The year

Kepler

P² = a³ in years and AU. How long a solar orbit takes, not how fast you leave.

The coast

Hohmann

Two burns and half an ellipse between two circular orbits. Earth to Mars is 258.88 days. Not a mission.

The ellipse

Vis-viva

Speed anywhere on one Keplerian ellipse. Earth’s perihelion rounds to 30.29 km/s. Not an ephemeris.

Neighborhood

Solar map

Where the eight planets sit. Day and local time, still a schematic.

The difference

Tides

The same pull, weaker on the far side. Two bulges, not a harbor table.