Example 1
M = 5.972e+24 kg, r = 6371000 m.
Enter the mass and the distance from the center. You get the field acceleration, with no falling mass in the formula. Earth at r = 6371 km is 9.82 m/s². At 400 km (r = 6771 km) you still have 8.69 m/s².
Force on a small mass: F = GMm/r². At constant g: free fall and Ep = m·g·h. In orbit compare with a = v²/r.
Constant G (N·m²/kg², optional), Mass M (kg) and Distance r (m). The result shows up here.
g = G·M/r² is the acceleration that mass M gives a small body at distance r. The test mass cancels, so a feather and a hammer fall together in vacuum. At Earth’s surface, M = 5.972×10²⁴ kg and r = 6.371×10⁶ m give g = 9.82 m/s².
Same numbers: G × M = 3.986×10¹⁴, divide by r² = 4.059×10¹³, you get 9.82. School 9.81 is a rounding. At 400 km altitude r grows to 6.771×10⁶ m and g only falls to 8.69 m/s². Astronauts did not “leave” the field.
Moon: M ≈ 7.35×10²² kg, r ≈ 1.737×10⁶ m, g ≈ 1.63 m/s², about one sixth of Earth’s. Mars at M ≈ 6.39×10²³ kg and r ≈ 3.390×10⁶ m is about 3.71 m/s². You type M and r. The calculator does the rest.
The same g goes into weight F = m·g and into Ep = m·g·h while g barely changes with height. On a circular orbit gravitational g equals centripetal acceleration v²/r. That is v₁ = √(GM/r).
M and r must be positive. Empty G = 6.67430×10⁻¹¹. The result is in m/s², or ft/s² with the US switch. A comma and a period in 5.972e24 are the same.
Falling under this g lives on h = ½gt² or t = √(2h/g). Here you stay with the field itself. Force on a chosen mass is next door: F = GMm/r².
g = G · M / r2
Default G = 6.67430×10−11. At Earth surface g ≈ 9.82 m/s2.
The field without a test mass: g = G·M/r². Earth at r = 6371 km is 9.82 m/s²; at 400 km (r = 6771 km) you still have 8.69 m/s².
M = 5.972e+24 kg, r = 6371000 m.
r ≈ 6771000 m (Earth + 400 km).
r ≈ 42164000 m.
M ≈ 7.35e+22 kg, r ≈ 1737000 m.
M ≈ 6.39e+23 kg, r ≈ 3390000 m.
r = 12742000 m.
M_☉ ≈ 1.989e+30 kg, r ≈ 149600000000 m.
M = solar mass, r = 10000 m.
G = 6.67e-11, Earth surface.
r = 6800000 m.
g = 9.82 m/s². At r = 6771 km (Earth plus 400 km) you get 8.69 m/s².
g is the acceleration from mass M. a = Δv/t is any speed change. In a drop with no drag, a ≈ g.
The station and you fall together along the orbit. Relative to the cabin the fictitious force vanishes, but the field is still there.
No. In g = GM/r² the test mass cancels. F = m g grows with m. The acceleration does not.
About 1.63 m/s² at M ≈ 7.35×10²² kg and r ≈ 1737 km. Mars at the surface is about 3.71 m/s².
F = m·g, or F = GMm/r² on the gravitational-force page. 70 kg and 9.82 m/s² is 687 N.
This calculator computes g from M and r. Type 9.81 as g on the free-fall pages, not here.
Yes. Type G in the field. Empty means 6.67430×10⁻¹¹.
At constant g use h = ½gt² or t = √(2h/g) on the fall pages.
r = 12,742 km, g drops by four, to about 2.45 m/s².
The formula is the school one. Units follow SI; NIST SP 330 and BIPM define the measures, not your result.
Page updated in 2026.