# How far away from Earth would we have to be so that an object released in space would not fall to Earth

Suppose we had a bowling ball that we took to space. Also suppose we stopped completely and released the ball. At which point would the gravitational pull of Earth be so weak that the ball would not fall towards Earth, but rather some other object?

I realize this might vary based on how close the Moon is, if there are asteroids and such with a stronger pull, but generally? I assume $$1\ 00\ 000 \ \mathrm{km}$$ would be close enough? What about $$\mathrm{1\ 000\ 000 \ km}$$? Is this question even solvable? Why / why not?

• This question already has an answer, it's r=³√(3GM/Λ/c²)=³√(GM/H²) see physics.stackexchange.com/a/531528/24093 Jun 11, 2020 at 19:02
• @Yukterez Ah, my knowledge of physics is limited, so I didn't know to search for that :) I have trouble understanding the solution, how much would that be in a more understandable form? Jun 11, 2020 at 19:14
• @Yukterez I really don't think that analysis was the spirit in which this question was asked. ;) Jun 11, 2020 at 19:17
• @Philip - I think it is, since it clearly reads "I realize this might vary based on how close the Moon is, if there are asteroids and such with a stronger pull, but generally?" with emphasis on "generally". Jun 11, 2020 at 19:24
• @Yukterez Ah, well, I suppose. It seemed to me, and this appears to have been confirmed by the OP, that the question was asked more in terms of simple Newtonian Gravity (not involving GR and cosmological constants). Jun 11, 2020 at 19:27

It depends what direction you're going, since gravity does have infinite range (as far as we know), so you need to know what other object it would be falling toward. If you are asking for the closest point at which an object would not fall toward the Earth, the Lagrange point $$L_1$$ of the Earth-Moon system is $$3.2639\cdot 10^8\ \mathrm m$$ away from the centre of mass of the Earth along the line from the Earth to the Moon, so anything just a little past this will fall toward the Moon. This point represents where the gravity of the Earth and Moon cancel out.