Weightless ≠ zero gravity
ISS astronauts still feel about 90% of Earth’s g; free-fall makes them float because they and the station constantly fall together.
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Gravity: For a (roughly) spherical body of mass M and radius R, gravitational acceleration at altitude h is g = G·M / (R + h)², where G = 6.67430×10⁻¹¹ m³·kg⁻¹·s⁻². Weight is W = m·g.
Newton’s Second Law: F = m·a. Provide any two of force, mass, and acceleration; the missing quantity is solved instantly.
| Body | g (m/s²) | Earth g |
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Gravity is the attractive interaction between objects that have mass or energy. It governs everything from a ball dropping to the ground to the choreography of planets, moons, and galaxies. In everyday terms, gravity is why you feel weight and why things fall when you let go. In physics terms, your weight is the force of gravity acting on your mass: W = m·g, where m is mass (in kilograms) and g is the local gravitational acceleration (in m/s²).
On (roughly) spherical worlds, gravity near the surface is well-approximated by g = G·M / (R + h)², where G is the gravitational constant, M is the body’s mass, R its mean radius, and h your altitude above the surface. Two immediate takeaways:
This is why astronauts in low Earth orbit feel weightless: they are in continuous free-fall around Earth. Gravity is still strong there; they’re just perpetually falling sideways fast enough to miss the ground—an orbit.
It’s common to mix up mass and weight. Mass is the amount of matter in an object and does not change when you travel. Weight is the gravitational force on that mass and does change with g. On Earth’s surface, standard gravity is about 9.80665 m/s². If a world’s surface gravity is 0.17 g (like the Moon), a 70 kg person would still have 70 kg of mass but would weigh only about 12%–17% of their Earth weight. Our calculator reports g in m/s² and in “Earth g” for quick comparisons.
Gravity provides a real-world context for Newton’s Second Law, F = m·a. When gravity is the only force acting, the acceleration you experience is simply a = g. Add other forces—like a rocket’s thrust, air resistance, or a spring—and the total acceleration comes from the vector sum of all forces divided by mass. This is why the same push (force) produces a smaller acceleration on a heavy object than on a light one.
Surface gravity depends on both mass and radius. A dense, compact body can have strong gravity even if it isn’t very massive, while a large, puffy world (like Saturn) can have moderate surface gravity despite enormous mass because its radius is so large. Our presets capture these differences so you can explore how weight and g vary from the Moon to Neptune—and beyond with custom mass and radius.
Try adjusting altitude in the tool to see how g changes with height, or switch bodies to compare your weight across the Solar System.
ISS astronauts still feel about 90% of Earth’s g; free-fall makes them float because they and the station constantly fall together.
On the Moon’s 1.62 m/s², a 700 N Earth weight drops to roughly 115 N—like holding a single grocery bag instead of your whole body.
Double the distance from a planet’s center and gravity weakens by 4×; triple it and you only feel 1/9 the pull.
Plugging F = m·a, a 10,000 N thruster accelerating a 2,000 kg stage gives 5 m/s² (~0.5 g)—handy when eyeballing launch numbers.
Even with 318 Earth masses, Jupiter’s surface gravity is only about 2.5 g because its radius is 11× bigger—mass and size both matter.