Do heavy things fall faster than light things?
― Galileo tested it on a ramp, not the Leaning Tower
"Heavier things fall faster." This idea was believed to be true for almost 2000 years. In reality, though, without air, heavy and light objects fall at exactly the same time. The people who proved it did so with a clever trick: they slowed the fall down so it could be measured.
Hold a thick book in one hand and a single sheet of notebook paper in the other, and drop both at once. The book thuds to the floor; the paper flutters down behind it. Heavier really does fall faster — or so it seems.
Now try dropping the paper resting on top of the book. The paper stays stuck to the book and falls right along with it. The paper wasn't lagging because it was light.
Now crumple the paper into a tight ball and drop it alongside the book. They land at almost the same instant. The paper's weight hasn't changed. What changed is how it catches the air.
There are only two reasons things of different weights fall together
A ball ten times heavier is pulled by Earth ten times more strongly. But something ten times heavier also takes ten times more force to get moving. Since the pull and the resistance to moving both scale up by the same factor, the two effects cancel out, and the speed builds up identically.
A falling object has to push air out of the way as it goes. Something like paper, with a lot of surface area for its weight, gets braked hard. Without air, even a feather falls at the same rate as a hammer.
Obvious as it sounds now, this was hard to prove. A fall takes only an instant, and people in earlier centuries had no clock precise enough to measure whether two things landed "at the same time."
Why was "heavier falls faster" believed for 2000 years?
Aristotle, in ancient Greece, held that heavier things fall faster. Compare a stone with a feather and that certainly seems true — because in everyday falls, air is always mixed into the picture.
In 1586, the Dutch scientist Simon Stevin and his colleague Jan Cornets de Groot recorded dropping two lead balls from a church tower, one ten times heavier than the other. The height was said to be about 9 metres, and the two balls were reported to hit the board below with what sounded like a single thud.
Italy's Galileo Galilei reached the same conclusion. The famous story of him dropping balls from the Leaning Tower of Pisa comes from a biography written by his student Vincenzo Viviani after Galileo's death. It appears nowhere in Galileo's own writings, and historians still debate whether it really happened.
Galileo slowed the fall down using a ramp
What Galileo actually documented was a far more painstaking experiment. He carved a straight groove into a board, tilted it, and rolled a bronze ball down it. On a slope, the ball still obeys the same rule, but falls slowly enough to observe.
He measured time by letting water trickle through a narrow tube from a container, then weighing the water that collected. This let him compare how far the ball travelled in each equal interval of time.
The result is shown in Figure 1. Taking the distance covered in the first interval as 1, the next interval covered 3, then 5, then 7 — increasing by odd numbers. The running totals from the start were 1, 4, 9, 16 — the square of the time elapsed. This pattern held no matter how heavy the ball was.
Galileo also argued against Aristotle with a thought experiment. Tie a heavy stone and a light stone together with a string and drop them. What happens?
If the light stone drags on the heavy one, the combined pair should fall slower than the heavy stone alone. But the pair together is also heavier than the heavy stone alone — so if "heavier falls faster" is true, the pair should also fall faster. Slower and faster at once is a contradiction, so he argued the original idea itself must be wrong.
How big a difference does air actually make?
Galileo was well aware of air's effect. In his book, he wrote that dropping a large iron ball and a small one from a height of about 60 metres produced a landing gap of only about two finger-widths. Air does cause some difference, he argued, but nowhere near the "difference proportional to weight" that Aristotle claimed.
The gap grows largest for things with a lot of surface area relative to their weight — paper, feathers, raindrops. A raindrop reaches a certain speed and then stops accelerating, falling at a constant rate from then on (explained in detail in why raindrops don't hurt).
In 1971, Apollo 15 astronaut David Scott dropped a hammer and a bird feather at the same moment on the Moon. As shown on the right of Figure 2, the two fell side by side and hit the ground together. Galileo's conclusion was confirmed live, on television.
Dropped from the same height, heavy and light objects reach the ground at almost the same speed. But the force of the impact is bigger for the heavier object. "Speed doesn't depend on weight" and "danger does depend on weight" are both true at once.
Summary
Heavier objects are pulled more strongly, but they're also proportionally harder to move, so falling speed doesn't depend on weight. Paper and feathers lag behind only because air is braking them. Galileo found this rule by slowing falls down on a ramp and timing them with a water clock.
Weight does not decide how fast something falls.
What undid a 2000-year-old assumption was a ramp and a water clock.
For how weight itself was ever measured, see how the Earth's weight was measured; for why your body feels lighter while falling, see why you feel lighter in an elevator.
- Take a book and a sheet of paper cut smaller than the book, and drop them separately at the same moment. Confirm the paper flutters down behind it.
- Next, drop the paper resting on top of the book. The paper should stay with the book and fall together, because the book pushes the air out of the way in front of it.
- Finally, crumple the paper into a tight ball and drop it alongside the book. Confirm they land at almost the same moment, even though the paper's weight hasn't changed.
When dropping the book, avoid your feet or anything breakable nearby, and drop it from a low height toward the floor.
Want to go deeper? ― Terms, formulas, and how this maps to textbooksFrom middle-school science to university-level courses, each level is labelled explicitly
- MSCovered in middle-school science
- HSCovered in high-school "Basic Physics" / "Physics"
- HS+High-school advanced content, or textbook sidebar material
- UnivNot covered in high school — university-level mechanics / general relativity
- ResearchNot yet settled even at university level — actively studied by researchers today
MSTerms: this phenomenon has names
- Free fall: motion of an object falling under gravity alone, when air effects can be ignored.
- Gravitational acceleration: the amount by which a falling object's speed increases each second. At Earth's surface, roughly 9.8 metres per second, every second.
- Air resistance: the force, opposite to the direction of motion, felt when pushing air out of the way.
- Inertia: an object's tendency to keep doing what it's already doing. This is why heavier things are harder to get moving.
MSHSWorking it out: how long would a drop from the Leaning Tower of Pisa take?
Let's calculate how long it would take to hit the ground if a ball really were dropped from the Leaning Tower, as legend says. We'll ignore air resistance as a small effect.
| In symbols | a = (m × g) ÷ m = g / h = ½ × g × t² so t = √( 2 × h ÷ g ) |
| In words | Falling acceleration = gravitational force ÷ mass = gravitational acceleration (mass cancels out). Falling time = the square root of "2 × height ÷ gravitational acceleration" |
| Where it comes from | Plugging a gravitational force proportional to mass into the equation of motion (force = mass × acceleration) cancels the mass out. Under constant acceleration, distance covered is proportional to the square of the elapsed time (the 1, 4, 9, 16 in Figure 1) |
| Drop height (near the gallery atop the leaning tower) | said to be about 56 m |
| Gravitational acceleration | 9.8 m/s² |
| Distance fallen in the first second (½ × g) | 4.9 m |
| Twice the height | 2 × 56 = 112 |
| Divide by gravitational acceleration (time squared) | 112 ÷ 9.8 ≒ 11.4 |
| Falling time | square root of 11.4 is about 3.4 seconds |
| Landing speed (m/s) | 9.8 × 3.4 ≒ 33 |
| Converted to km/h | 33 × 3.6 ≒ 119 |
| Distance fallen in the 2nd second | 4.9 × 3 = 14.7 |
| Distance fallen in the 3rd second | 4.9 × 5 = 24.5 |
A ball dropped from the top of the leaning tower would take about 3.4 seconds to hit the ground, reaching a speed of about 120 km/h. The distance covered each second — 4.9, 14.7, 24.5 metres — grows in the ratio of odd numbers 1, 3, 5, the same rule as the ramp in Figure 1. Notice the ball's weight never appears anywhere in this calculation. That's what "doesn't depend on weight" means.
HSHS+What changes when air resistance is included?
HSIn high-school physics, falling is first taught as "uniformly accelerated straight-line motion" ignoring air resistance. The 1, 3, 5, 7 pattern follows from speed increasing in proportion to time.
HS+Air resistance scales with cross-sectional area for a given shape, while weight (for a given material) scales with volume. Double the size and the cross-section grows fourfold while the weight grows eightfold, so the braking effect per unit weight is halved. Bigger, heavier balls are less affected by air, and reach a higher "terminal velocity."
UnivWhy are the "strength of pull" and "resistance to moving" exactly equal?
The mass that determines how strongly gravity pulls an object (gravitational mass) and the mass that determines how hard it is to move (inertial mass) being equal is not actually something that falls out of theory — it's a fact confirmed by experiment. This is called the equivalence principle, and its precision has been refined through experiments such as the Eötvös experiment. Einstein took this as the starting point for building general relativity.
📖 For the full derivation and further reading: Equivalence principle (Wikipedia, Japanese)
ResearchWhat's still not fully settled
- Did Galileo really drop anything from the leaning tower? With no record from Galileo himself, and the story appearing only in his student's biography, historians remain divided.
- How precisely does the equivalence principle hold? Satellite-based experiments report finding no deviation, however tiny. Any deviation found would be a trigger to rebuild our theory of gravity.
- Does antimatter fall the same way? In 2023, antihydrogen atoms were observed falling downward for the first time. Whether the way they fall is exactly identical to ordinary matter, though, is still being examined with increasing precision.
In other words, even this article describes things "as far as we currently understand them." The rule discovered on a ramp 400 years ago is still being tested in cutting-edge experiments today.
How this maps to textbooks (by level)
| Level | Subject / unit | Where in this article |
|---|---|---|
| MS | Science ― Motion and energy (motion down a slope) | The ramp experiment, speed steadily increasing |
| HS | Basic Physics ― free fall, equation of motion | Calculating falling time and landing speed |
| HS+ | Physics ― air resistance and terminal velocity | Why paper and feathers lag behind |
| Univ | Mechanics ― general relativity | Gravitational mass, inertial mass, the equivalence principle |
| Research | Precision gravity experiments ― antimatter physics | Testing the equivalence principle, antihydrogen's fall |
| ― | Everyday connection | Same falling speed, but impact force changes with weight |
- Galileo Galilei, Discorsi e Dimostrazioni Matematiche Intorno a Due Nuove Scienze (Japanese edition trans. Takeo Konno and Setsuji Hida, Iwanami Bunko)
- Simon Stevin, De Beghinselen der Weeghconst (1586), appendix describing the falling-body experiment
- NASA ― The Apollo 15 Hammer-Feather Drop
- Anderson et al., "Observation of the effect of gravity on the motion of antimatter," Nature 621 (2023)
※This article is a general-audience science explainer. The figures given are approximations meant to aid understanding, not precise values. Accounts of the historical experiments vary between sources in their details.