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Physics · the force that shapes the universe

Gravity

The weakest of nature's forces runs the cosmos. Why an apple and the Moon obey the same rule, and why Einstein said gravity is not a force at all.

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Explained like you're twelve. Explained like you've just finished school. Explained like you're at university.

Physics · Newton 1687 · Einstein 1915

Mass tells space how to bend; space tells mass how to move.

Launch the body sideways and watch the same law draw every kind of orbit. Too slow and it falls into a tight ellipse. At exactly circular speed it traces a circle. Faster and the ellipse stretches out. Push past about 1.41 times circular speed and it reaches escape speed and never comes back.

Drop anything and it falls. Throw it harder and it travels further before it lands. Throw it hard enough and it never lands at all. Instead it falls around the Earth in a great circle, which is exactly what the Moon is doing. An orbit is just falling that keeps missing the ground.

Gravity is the pull that every lump of matter has on every other lump. The more mass something has, the stronger its pull. The further away you get, the weaker that pull becomes. The Earth is huge, so it holds you to the ground and keeps the Moon circling us. The Sun is far bigger, so it keeps every planet looping around it.

Isaac Newton's great idea, more than three hundred years ago, was that all of this is one thing. The apple dropping from the tree and the Moon sweeping across the sky obey a single rule. That one law explains the tides, the arc of a thrown ball, and the path of every planet in the sky.

Centuries later Einstein found something stranger underneath it. Gravity, he said, is not really a force tugging you downward. It is what you feel as you move through a space and time that a nearby mass has bent out of shape. We will build up to that idea below.

Newton's law of universal gravitation puts numbers on the pull. Any two masses attract each other with a force that grows with each mass and shrinks with the square of the distance between them:

\[ F = G\,\frac{m_1 m_2}{r^2}. \]

That inverse-square part is the heart of it. Double the distance and the pull drops to a quarter. Triple it and it drops to a ninth. The same falling-off shapes everything from a tossed ball to a comet's long loop.

The constant \(G\) is tiny, which is why gravity feels so weak. A small fridge magnet can hold a paperclip against the pull of the entire planet. Gravity only takes over at large scales because, unlike the magnet, it never cancels out. Pile up enough mass and it wins.

The orbit sandbox above is this law doing its work. A body launched sideways is always falling toward the star, but its sideways motion keeps carrying it past. Get the speed just right and the curve of its fall matches the curve of the star, and you have a circle. The circular speed at a radius \(r\) is \(v_c=\sqrt{GM/r}\). Launch slower and the body swings in closer on a tight ellipse. Launch faster and the ellipse stretches outward. Reach \(\sqrt{2}\,v_c\), the escape speed, and the path opens up forever and the body leaves for good.

Newton's law is astonishingly accurate. It landed probes on other planets and predicted the existence of Neptune before anyone saw it. But it left two things unsaid. It never explained what gravity actually is, only how strong it is, and Newton himself was uneasy that it reached across empty space instantly. And by the late 1800s it was known to get one thing slightly wrong: the slow turning of Mercury's orbit was off by a tiny amount no one could account for.

Geometry, not force. Einstein's general relativity, published in 1915, recast gravity entirely. Mass and energy tell spacetime how to curve, and the curved geometry tells matter how to move. A planet circling the Sun is not being pulled on a string. It is coasting along the straightest path available, a geodesic, through a region of spacetime the Sun has warped. John Wheeler put the whole theory in one line: matter tells space how to bend, and space tells matter how to move.

The equivalence principle. The seed of the idea is simple. Standing on the floor of a sealed room on Earth feels exactly like standing in a rocket accelerating through deep space, and floating in orbit feels exactly like floating far from any mass. Gravity and acceleration are locally the same thing. That is why everything falls at the same rate, a hammer and a feather together in a vacuum, since they are not being pushed by a force that depends on their mass. They are simply following the same curved geometry.

What Newton missed. General relativity reproduces Newton's law wherever gravity is weak, then adds small corrections that turn out to be exactly right. It accounts for the leftover drift in Mercury's orbit, about 43 arcseconds per century. It predicted that starlight would bend as it grazed the Sun, confirmed during the 1919 eclipse, and that clocks run slower deeper in a gravitational well, a shift your phone's GPS has to correct for every day.

Ripples in spacetime. If mass curves spacetime, then violently moving mass should send out ripples in it. In 2015 the LIGO detectors caught one: a gravitational wave from two black holes that spiralled together and merged more than a billion years ago, stretching every length on Earth by less than the width of a proton as it passed. A century-old prediction, finally heard.

The unfinished part. For all that, gravity is the force we understand least at the smallest scale. General relativity and quantum mechanics are each superbly tested, yet they refuse to combine. Where both must apply at once, inside a black hole or at the first instant of the Big Bang, the equations give nonsense. A working quantum theory of gravity, whether from strings, loop quantum gravity, or something not yet imagined, is still the largest open problem in physics. Gravity is the force we know best across the cosmos and least in the small.

Related: Relativity: Special & General · next: Black Holes & the Event Horizon · or go back to all topics.