Gravity Through Contradiction

A thought experiment about falling bodies

If heavier bodies fall faster, tying a light body to a heavy one must make the pair fall both slower and faster than the heavy body alone.

That impossible prediction is enough to break the rule. The reasoning does not require a dangerous jump, a tall tower, or a precision clock. A park bench, two pairs of shoes, and a child willing to ask one more question will do.

The Apple That Waited

The leaves had turned orange, but one apple still held to a branch above the park bench.

Bill and Teddy had walked far enough. Bill set his gray knapsack on the ground and sat. Teddy climbed onto the seat beside him—not to jump, only to gain the excellent authority that comes from being ten years old and a little taller than one’s father.

Bill’s red shoes rested on the path. Teddy’s white shoes swung above them.

“Heavy things fall faster,” Teddy said. A yellow leaf performed a long, wandering descent behind him. “That leaf is light. You are heavy. You would fall fast.”

“That sounds right,” Bill said. “Let us see whether the rule can survive its own consequences.”

Two Bodies, Side by Side

Bill pointed to their shoes.

“Imagine one red shoe and one white shoe begin falling side by side from the same height. Your rule says the heavier red shoe gets to the ground first.”

“Of course.”

“Now imagine a loose string joining them. The white shoe is the slower one. What does a slower thing do to a faster thing when they are tied together?”

Teddy pulled one hand back with the other. “It slows it down.”

“Then the joined pair must fall more slowly than the red shoe alone.”

“Yes.” Teddy paused. He could hear a bicycle freewheel clicking somewhere behind the trees.

Bill continued. “But the joined pair is heavier than the red shoe alone.”

“So it has to fall faster.”

“Faster and slower?”

Teddy frowned at the shoes as if one of them had cheated. “It cannot do both.”

Then Teddy improved the picture. “Use us. You weigh 150 pounds. I was 95 in July.”

“Together?”

Teddy counted, lost his place, and started again. “Two hundred forty-five pounds!” He was delighted by the size of the answer and hugged his father as if completing the addition required joining the bodies physically.

In the imagined fall, holding Bill’s hand would make Teddy part of the heavier combined body, so the old rule says they must fall faster than Bill alone. But if lighter Teddy is the slower body, the same handhold should retard Bill and make the pair fall more slowly. The human version and the shoes produce the same contradiction without anybody leaving the bench.

The Rule Defeats Itself

Put the reasoning in order:

  1. Assume a heavier body falls faster than a lighter body.
  2. Join a light body to a heavy body.
  3. Because the light body is slower, it should retard the heavy body. The pair should fall more slowly than the heavy body alone.
  4. Because the pair is heavier than the heavy body alone, the original rule also says the pair should fall faster.
  5. The same pair cannot be both slower and faster than the same comparison body, in the same conditions and at the same time.
  6. Therefore the starting rule is inconsistent.

The important move is not measuring which shoe wins. It is following the assumed rule until the rule gives two incompatible answers.

This is a Galileo-style reductio ad absurdum: assume the claim, derive a contradiction, and reject the assumption that produced it. The contradiction uses the principle of noncontradiction. It is not an example of the law of excluded middle.

“But I Have Seen Heavy Things Win”

Teddy pointed at the leaf, which had finally landed.

“An apple gets down before a leaf. I can see that.”

“Yes,” Bill said. “The air gets a vote.”

A falling object pushes air out of its way. The air pushes back. Shape, area, orientation, speed, and density all matter. A broad leaf can experience a large drag force compared with its weight. It flutters, rotates, and catches new air. A compact apple pushes through more steadily.

Change the shape and the result changes. A flat sheet of paper falls slowly. Crumple the same sheet into a small ball and it falls much faster through the same room, even though its mass is essentially unchanged.

Remove the air and the distinction disappears. At the same location in an ideal vacuum, bodies released with the same initial motion have the same gravitational acceleration regardless of their mass. Near Earth, that acceleration is approximately constant over modest height differences.

The thought experiment does not claim that every object reaches the ground at the same time in every ordinary situation. It isolates gravity from the other forces that ordinary situations add.

Mass Cancels in the Acceleration

The same result appears in the familiar equations.

Near Earth’s surface, the gravitational force on an object with gravitational mass mg is approximately:

F = m_g g

Newton’s second law relates net force to inertial mass mi and acceleration:

F = m_i a

If gravity is the only significant force, combine them:

m_i a = m_g g
      a = (m_g / m_i) g

Experiment tells us that gravitational and inertial mass are proportional with extraordinary precision. In the usual choice of units their ratio is one, so a = g. A larger mass experiences a larger gravitational force and also requires proportionally more force for the same acceleration; its mass does not remain in the final acceleration.

Air resistance adds another force whose scaling is different. That is why real leaves, feathers, raindrops, shoes, and apples can fall differently without rescuing the rule that gravity accelerates heavier bodies more.

The Difference Between a Bad Observation and a Bad Inference

“So people were foolish?” Teddy asked.

“No. The observation was real. Stones often beat leaves. The inference was too quick.”

Experience arrives with several causes mixed together. Gravity, drag, buoyancy, wind, shape, and rotation contribute to one visible motion. If we name the largest-looking object as the only cause, we can build a rule that works in familiar cases and fails as soon as the cases are recombined.

The joined-body argument is powerful because it does not merely present a surprising counterexample. It shows that the rule cannot assign a coherent outcome to a system made from the very bodies it claims to describe.

That technique travels well beyond mechanics. When evaluating a proposed rule, compose two cases and ask whether the rule still gives one answer. Check the whole made from the parts. Follow every consequence, including the consequence that points in the opposite direction.

The Apple Finally Falls

A black bird landed on the branch above the bench. The branch moved. The last apple dropped into the grass with a soft thud.

Teddy looked at the leaf on the path and the apple under the tree.

“The apple won.”

“In air, with those shapes.”

“In a vacuum, the leaf wins too?”

“There is no winner. They keep pace.”

Teddy nodded, then looked again at the red and white shoes.

“The string broke the rule.”

“The string only made the contradiction easy to see.”