Everyday Mysteries Mechanics No background needed ~7 min read

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.

Published: 2026.09.23 Difficulty: ★☆☆ (no background needed) Formulas appear only in the final collapsible section
Picture this first

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

1
Heavier things are harder to move — by exactly the same amount

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.

2
The real difference-maker is air

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.

Ball position at equal time intervals (Galileo's ramp experiment) 0 Beat 1 Beat 2 Beat 3 Beat 4 1 3 5 7 Numbers below slope = distance per beat (grows as odd numbers 1 : 3 : 5 : 7) Total distance from start 1 → 4 → 9 → 16 = proportional to time squared Time measured with a water clock. Ratio unchanged even with a heavier ball
Figure 1: Position of the ball rolled from the upper left, at equal time intervals ("beats"). The numbers below the slope are the distance covered per beat: 1, 3, 5, 7 — growing as odd numbers. The running total from the start is 1, 4, 9, 16 — the square of the time elapsed.

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).

Left: Earth, with air Right: airless Moon (1971) Dashed line = height at release Dashed line = height at release Iron ball Feather Braked by air Hammer Feather Fall side by side, same height
Figure 2: On the left, on Earth, the feather is left behind even when released at the same moment. On the right, on the airless Moon, the hammer and feather fell together at the same height. Downward arrows show the direction of fall.

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.

💡 Same falling speed, different story on impact

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.

🧪 Confirm Galileo's conclusion with a single sheet of paper
  1. 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.
  2. 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.
  3. 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
How to read the labels below
  • 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

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.

⓪ The underlying formula
In symbolsa = (m × g) ÷ m = g / h = ½ × g × t² so t = √( 2 × h ÷ g )
In wordsFalling acceleration = gravitational force ÷ mass = gravitational acceleration (mass cancels out). Falling time = the square root of "2 × height ÷ gravitational acceleration"
Where it comes fromPlugging 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)
① Starting figures
Drop height (near the gallery atop the leaning tower)said to be about 56 m
Gravitational acceleration9.8 m/s²
Distance fallen in the first second (½ × g)4.9 m
② Working through the numbers
Twice the height2 × 56 = 112
Divide by gravitational acceleration (time squared)112 ÷ 9.8 ≒ 11.4
Falling timesquare root of 11.4 is about 3.4 seconds
Landing speed (m/s)9.8 × 3.4 ≒ 33
Converted to km/h33 × 3.6 ≒ 119
Distance fallen in the 2nd second4.9 × 3 = 14.7
Distance fallen in the 3rd second4.9 × 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

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)

LevelSubject / unitWhere in this article
MSScience ― Motion and energy (motion down a slope)The ramp experiment, speed steadily increasing
HSBasic Physics ― free fall, equation of motionCalculating falling time and landing speed
HS+Physics ― air resistance and terminal velocityWhy paper and feathers lag behind
UnivMechanics ― general relativityGravitational mass, inertial mass, the equivalence principle
ResearchPrecision gravity experiments ― antimatter physicsTesting the equivalence principle, antihydrogen's fall
―Everyday connectionSame falling speed, but impact force changes with weight
References
  1. Galileo Galilei, Discorsi e Dimostrazioni Matematiche Intorno a Due Nuove Scienze (Japanese edition trans. Takeo Konno and Setsuji Hida, Iwanami Bunko)
  2. Simon Stevin, De Beghinselen der Weeghconst (1586), appendix describing the falling-body experiment
  3. NASA ― The Apollo 15 Hammer-Feather Drop
  4. 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.