Editing Orbit (section)

===Illustration===
{{main|Newton's cannonball}}
[[File:Newton Cannon.svg|thumb|300px|[[Newton's cannonball]], an illustration of how objects can "fall" in a curve]]

As an illustration of an orbit around a planet, the [[Newton's cannonball]] model may prove useful (see image below). This is a '[[thought experiment]]', in which a cannon on top of a tall mountain is able to fire a cannonball horizontally at any chosen muzzle speed. The effects of air friction on the cannonball are ignored (or perhaps the mountain is high enough that the cannon is above the Earth's atmosphere, which is the same thing).<ref>See [https://books.google.com/books?id=rEYUAAAAQAAJ&pg=PA6 pages 6 to 8 in Newton's "Treatise of the System of the World"] {{Webarchive|url=https://web.archive.org/web/20161230132051/https://books.google.com/books?id=rEYUAAAAQAAJ&pg=PA6 |date=30 December 2016 }} (written 1685, translated into English 1728, see [[Philosophiæ Naturalis Principia Mathematica#Preliminary version|Newton's 'Principia' – A preliminary version]]), for the original version of this 'cannonball' thought-experiment.</ref>

If the cannon fires its ball with a low initial speed, the trajectory of the ball curves downward and hits the ground (A). As the firing speed is increased, the cannonball hits the ground farther (B) away from the cannon, because while the ball is still falling towards the ground, the ground is increasingly curving away from it (see first point, above). All these motions are actually "orbits" in a technical sense—they are describing a portion of an elliptical path around the center of gravity—but the orbits are interrupted by striking the Earth.

If the cannonball is fired with sufficient speed, the ground curves away from the ball at least as much as the ball falls—so the ball never strikes the ground. It is now in what could be called a non-interrupted or circumnavigating, orbit. For any specific combination of height above the center of gravity and mass of the planet, there is one specific firing speed (unaffected by the mass of the ball, which is assumed to be very small relative to the Earth's mass) that produces a [[circular orbit]], as shown in (C).

As the firing speed is increased beyond this, non-interrupted elliptic orbits are produced; one is shown in (D). If the initial firing is above the surface of the Earth as shown, there will also be non-interrupted elliptical orbits at slower firing speed; these will come closest to the Earth at the point half an orbit beyond, and directly opposite the firing point, below the circular orbit.

At a specific horizontal firing speed called [[escape velocity]], dependent on the mass of the planet and the distance of the object from the barycenter, an open orbit (E) is achieved that has a [[parabolic trajectory|parabolic path]]. At even greater speeds the object will follow a range of [[hyperbolic trajectory|hyperbolic trajectories]]. In a practical sense, both of these trajectory types mean the object is "breaking free" of the planet's gravity, and "going off into space" never to return.