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Gravity and Orbits

Astronauts float where Earth's gravity is still strong. What is actually missing?

Fire Newton's cannon yourself, find out why astronauts float even though gravity is still strong, and see why speeding up can leave a spacecraft moving more slowly.

Space guide 8 min read
Astronauts float where Earth's gravity is still strong. What is actually missing? — original ExplainItSimply topic illustration

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An orbiting spacecraft and its occupants are falling together. Because the floor is not holding them up as it does on Earth, they experience apparent weightlessness.

Enough sideways speed makes the falling path curve around Earth. A spacecraft does not need to escape gravity to orbit; gravity is what bends its journey.

Build the physical explanation of a curved path from velocity and gravity, then test a simple orbital relationship. The related orbit story applies that mechanism to the puzzle of travelling without continually firing an engine.

A strange number to start with

Right now, the Moon is falling toward you by about 1.4 millimetres every second.

It never arrives. In that same second it also moves about a kilometre sideways, and Earth's surface curves away beneath it by almost exactly the amount it has fallen. That is all an orbit is: falling and missing. The same idea explains why astronauts float, why satellites stay up, why your phone knows where you are, and why a day on a space station feels like free-fall, because it is.

Try it before you read it

Fire a cannonball and watch gravity decide its fate

In the 1680s Isaac Newton imagined a cannon on a very tall mountain, firing horizontally. Fire it slowly and the ball drops to the ground nearby. Fire it faster and it lands farther away. Keep going and something remarkable happens: the ground curves away as fast as the ball falls. Use the slider to run Newton's experiment. The planet here is Earth-sized and the air has been removed, so only gravity acts.

Newton's cannon

Launch speed: 7.9 km/s

Pause and think

At 7.9 km/s the ball goes round in a circle. A little faster, 8.5 km/s say, and it traces a stretched oval that flies far from Earth. Why does more speed at the start make the ball spend less time near the planet later? Test your guess with the slider.

The moment it clicked for Newton

The same force that drops an apple holds the Moon

The story of the apple is probably tidied up, but the idea behind it is real. Newton asked whether the force that pulls things to the ground might reach all the way to the Moon, only weaker. He knew the Moon is about 60 times farther from Earth's centre than an apple is. If gravity weakens with the square of distance, the pull there should be 60 × 60 = 3,600 times smaller than at the surface.

Do the sum. Surface gravity pulls things down at 9.8 metres per second, every second. Divide by 3,600 and you get about 0.0027, which makes the Moon fall roughly 1.4 mm each second. Newton compared that to how much the Moon's path actually bends and found they matched. The ground and the sky, which people had treated as separate worlds for thousands of years, obeyed one rule.

Planet 1× distancepull = 1 2× distancepull = ¼ 3× distancepull = 1⁄9

Is an orbiting astronaut floating because Earth's gravity has disappeared?

Orbit combines inward gravitational acceleration with sideways motion.

Trace the explanation

An astronaut and the spacecraft follow nearly the same free-fall path, so the floor does not provide the usual support force. Gravity is still central to that motion.

Source and further reading: NASA

The biggest misunderstanding in space

Astronauts are not floating because there is no gravity

What most people think

Above the atmosphere there is no gravity, so astronauts float and satellites hover.

What is actually true

At the International Space Station's height of about 400 km, gravity is still roughly 90% as strong as on the ground. The crew float because the whole station is in free-fall, along with everything inside it.

Picture being in a lift whose cable snaps. You and the lift fall together, so you would drift weightlessly inside it even though gravity is working fully. The ISS is that lift, except it also moves sideways at about 7.7 km/s, or about 27,600 km/h. It falls constantly and constantly misses Earth, completing a lap in about 92 minutes. The crew see around 16 sunrises every day.

~7.7 km/sISS speed, fast enough to cross the Atlantic in about 12 minutes
~90%of surface gravity felt at the ISS's altitude
35,786 kmheight of a geostationary orbit, where one lap takes a full day

An astronaut can feel weightless while gravity remains strong

A spacecraft in orbit is continually falling toward Earth while moving sideways fast enough that its path curves around the planet. Its occupants and loose objects fall together. A scale measures the support force beneath you, so a freely falling scale can read almost zero without gravity disappearing.

This distinction separates gravitational pull from the sensation of weight. Standing on the ground, you feel the ground pushing you upward. In a freely falling cabin that support is missing, even though gravity keeps changing the cabin's motion.

Gravity changes the direction of sideways motionA satellite on a circular path has an instantaneous velocity tangent to the orbit. Gravity points inward toward Earth. The two arrows are different kinds of quantity and their lengths are not comparable scales.Falling and moving sidewaysVelocity at this pointGravityEarthDirections shown; size and arrow lengths are illustrative.
A rule that feels wrong

To catch a satellite ahead of you, you slow down, not speed up

Orbits behave in ways that trick everyday intuition. Higher orbits are slower, not faster, because gravity is weaker there and less sideways speed is needed to keep missing. Yet to reach a higher orbit, a spacecraft has to fire its engine forward to speed up. Here is what happens next:

  1. The spacecraft speeds up with a short burn, so its path stretches into an oval that rises on the far side of Earth.
  2. As it climbs, it trades speed for height and slows down, just like a ball thrown upward.
  3. At the top of the oval it fires again to round the path into a new circle, now at a higher altitude and moving slower than before.
Burn 1: speed up Burn 2:circularise Final orbit: higher, slower Starting orbit: lower, faster (inner circle)
Where gravity quietly runs your day

Tides, satellites and the reason your phone knows where you are

Tides

The Moon pulls harder on the side of Earth facing it than on the far side. That difference stretches the oceans into two bulges as Earth turns through them, giving most coasts two high tides a day. See The Moon for the full picture.

Satellites

Hundreds of weather, communication and navigation satellites each follow the cannonball rule at different heights. Low ones circle in about 90 minutes. Geostationary ones match Earth's spin and appear fixed over one spot, which is why a satellite dish can stay pointed at one place.

GPS and time itself

GPS satellites orbit at about 20,200 km. Their clocks run slightly fast because gravity is weaker there, and slightly slow because they move quickly. Engineers must correct the net difference of roughly 38 microseconds a day, otherwise position errors would pile up by kilometres daily.

The deeper answer

Newton told us how gravity behaves. Einstein suggested what it is.

Newton's formula predicts orbits superbly, but he admitted he did not know why masses attract one another. In 1915 Albert Einstein proposed general relativity: mass and energy bend space and time, and objects follow the straightest possible path through that bent space. A planet orbits not because a string pulls it but because the space around the Sun is curved.

A common picture is a heavy ball sinking into a stretched rubber sheet while marbles roll around it. It is a helpful image with a flaw, because on a sheet "down" is itself caused by gravity. The real bending involves time as well as space, which is why GPS clocks need correcting.

  • 1687: Newton publishes his law of universal gravitation in the Principia.
  • 1798: Henry Cavendish weighs the Earth indirectly by measuring the tiny attraction between lead balls.
  • 1915: Einstein publishes general relativity.
  • 1919: Starlight is seen bending around the Sun during an eclipse, matching Einstein's prediction.
  • 1957: Sputnik 1 becomes the first artificial satellite.
  • 2015: LIGO detects gravitational waves, ripples in space-time from colliding black holes.

How do you time a lap when space has no painted starting line?

Choose a reference, such as returning to the same direction relative to distant stars. A period is the elapsed time between equivalent positions under that definition.

A calendar based on the Sun uses a different reference. That is why one Earth rotation relative to the stars is slightly shorter than the average sunrise-to-sunrise day.

One sideways push changes the entire path

Imagine releasing a ball from a hill, then launching it sideways faster and faster in a simplified world with no air or obstacles. At low speed it lands nearby; with enough sideways motion, Earth's curved surface falls away beneath it. This is an illustration of orbital motion, not an instruction for a real launch.

Increasing speed does not always mean settling into a higher circular orbit immediately. A burn usually changes the shape of a path; another burn may be needed to make it circular. Mission design tracks position, velocity and fuel together rather than selecting a distance and hoping the spacecraft stays there.

The same rule at different heights

Three orbits that quietly run modern life

Because orbital speed depends on height, each altitude gives satellites a different job. Here are the three families you rely on, with the numbers that define them.

OrbitTypical heightTime for one lapUsed for
Low Earth orbit400 to 2,000 kmabout 90 to 130 minutesSpace station, Earth imaging, many internet satellites
Medium Earth orbitabout 20,200 kmabout 12 hoursGPS and other navigation systems
Geostationary orbit35,786 km23 h 56 min (one Earth spin)Weather and TV satellites that stay above one place

Notice that the higher the orbit, the longer the lap. That is Kepler's rule in action, found by studying planets centuries before spacecraft existed: the farther out, the slower the pace. It is also why a satellite in geostationary orbit must be exactly 35,786 km up. At any other height its lap would not match Earth's rotation.

Stealing speed from a planet

The slingshot that took Voyager to the edge of the Solar System

A spacecraft cannot carry enough fuel to reach Neptune quickly. Instead, mission planners use gravity assists. As a probe swings close to a moving planet, gravity bends its path, and the probe gains a little of the planet's orbital speed. The planet slows by an immeasurably small amount, since it is billions of billions of times heavier.

Voyager 2 used this trick at Jupiter, Saturn and Uranus on the way to Neptune. That journey was only possible because, in the late 1970s, the four giant planets were arranged in a favourable sweep, an alignment that comes around roughly once every 175 years. Miss it, and the same trip would have needed far more fuel or decades more time.

Why would simply turning off a spacecraft engine not usually make it drop vertically out of orbit?

One reasoned response

It retains its sideways velocity. A change in orbit requires a change in motion; atmospheric drag and engine burns can provide that change. Coasting is not the same as stopping.

Source and further reading: NASA

Pause and think

A gravity assist seems to break the rule that you cannot get energy for free. It does not: the energy comes from the planet's motion around the Sun. The planet is slowed, just very slightly, as the probe speeds up.

Gravity is not even the same everywhere on Earth

Why you weigh slightly less at the equator than at the poles

The number 9.8 m/s² is an average. At the poles it is about 9.83, and at the equator about 9.78. Two things cause this: Earth bulges at the equator, so you are a little farther from the centre, and the spin reduces your effective weight there. The difference is about half a percent, so a 70 kg person would read around 0.35 kg lighter at the equator. Mountains, ocean trenches and the rock beneath you also change it very slightly, and satellites can map those differences to study the planet's interior and ice sheets.

At the other extreme is gravity so strong that nothing escapes. A black hole is a region where the escape velocity exceeds the speed of light. If the Sun were swapped for a black hole of the same mass, Earth would continue in its orbit exactly as before, though it would be a cold, dark place.

Predict an orbit before trusting the animation

For objects orbiting the same central mass, larger orbits usually have longer periods. The Sun-orbit calculator uses Kepler's relation for small orbiting bodies; enter 1 AU and then 4 AU to see the period change from 1 to 8 Earth years.

The relationship does not say every object in space obeys that exact AU formula. A moon orbiting a planet has a different central mass. A close encounter, atmospheric drag or another body's influence can also make the simple two-body model inadequate.

Compare orbital size with the length of a year

Period in Earth years = AU raised to 1.5. This simplified two-body relationship is not a satellite-around-Earth calculator.

Enable JavaScript to calculate; the assumptions are explained above.
Would switching off a spacecraft's engine make it stop moving?

No. In the absence of a force that changes its motion, it continues moving. Engines change velocity; they are not required simply to preserve motion through space.

Three tests you can do today

Feel orbits with things you already own

  1. The bucket swing. Put a little water in a bucket with a sturdy handle and swing it in a fast vertical circle, outdoors. The water stays inside at the top because the bucket is falling away from it at the same time. This is the same falling-and-missing as an orbit.
  2. The paper and the book. Drop a book and a flat sheet of paper together: the book wins. Now place the paper on top of the book and drop both: they fall together. Air resistance, not weight, made the difference.
  3. The ball on a string. Whirl a small ball on a string. The string plays the role of gravity, pulling the ball inward. Let go, and the ball moves off in a straight line, just as a planet would if the Sun's pull vanished.

Keep following the thread

See gravity organise a whole family of worlds in The Solar System, or find out how it creates tides and keeps one face of the Moon pointed at us in The Moon.

Gravity questions that trip people up

Does a heavier object fall faster?

In a vacuum, no. All objects accelerate at the same rate regardless of mass. On Earth, air resistance makes a feather fall slower than a hammer, but on the Moon, astronauts showed both hitting the ground together.

What is escape velocity?

It is the speed needed to climb away from a planet without further engine power. For Earth's surface it is about 11.2 km/s. Try the cannon above 11.2 km/s and the path never returns.

Could gravity ever be switched off?

Nothing known shields against gravity. Weightlessness comes from free-fall, not from escaping gravity.

Why is gravity so weak compared with magnets?

A small fridge magnet can lift a paperclip against the pull of the entire Earth. Gravity only wins at large scale because it always attracts and never cancels out, while electric and magnetic effects usually balance.

Sources

Sources and further reading

A closer look

Falling can curve around a world

Imagine successive positions of an orbiting object. Its forward motion carries it onward while gravity continually changes its direction toward the central body.

Work through the distinction

An orbit is not a place where gravity switches off. Astronauts and their nearby spacecraft fall together, producing the experience of weightlessness. The simplified picture leaves out atmospheric drag and other bodies.

Gravity curves motion; it does not switch off: Conceptual circular-orbit sketch. Object sizes and separation are not to scale.

Does orbit require gravity to vanish?

Choose an answer to see feedback. You can try again.

Show the answer and explanation

No, gravity helps curve the motion. An orbit is not a place where gravity switches off. Astronauts and their nearby spacecraft fall together, producing the experience of weightlessness. The simplified picture leaves out atmospheric drag and other bodies.

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Watch the same orbital idea work at different scales

An orbit combines motion with a continuing gravitational pull. Apply that idea to planets around the Sun, then see how space missions use careful measurements to plan journeys between worlds.