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Ladder paradox

Adapted from Wikipedia · Adventurer experience

A scientific diagram illustrating the concept of spacetime and the ladder paradox in physics.

The ladder paradox (or barn-pole paradox) is a thought experiment in special relativity. It uses a ladder moving very fast, close to the speed of light. Because it moves so fast, it gets shorter. This is called Lorentz length contraction.

Imagine a garage that is shorter than the ladder when the ladder is not moving. If the ladder were not moving, it would not fit inside the garage. But when the ladder moves very fast, it looks shorter to someone standing still. To this person, the ladder can fit inside the garage.

But for someone moving with the ladder, the ladder looks its normal length. To them, the garage looks shorter. So they think the ladder cannot fit inside the garage.

This seems like a problem, but it is not really. The issue comes from thinking that things happening at the same time for one person happen at the same time for everyone. In special relativity, simultaneity is relative. This means what looks like it happens at the same time for one person might not for another. This explains why the two observers see things differently.

Paradox

Imagine a garage with open front and back doors, and a ladder that is too long to fit inside when both doors are closed. If we move the ladder very fast through the garage, something interesting happens. Because it is moving so quickly, the ladder appears to become shorter due to a rule in physics called length contraction. For a moment, the ladder can fit completely inside the garage, and we could even close both doors at the same time to trap it inside.

But here’s where things get puzzling. If we look from the ladder’s point of view, it seems like the ladder is still its normal length, and instead, the garage is moving and appears shorter. From this angle, the garage looks too small to ever hold the whole ladder. This clash of viewpoints creates what we call the ladder paradox.

Resolution

The solution to the ladder paradox comes from the idea of the relativity of simultaneity. This means that what one person thinks happens at the same time might not be the same time to someone else moving very fast.

Imagine you have a garage and a ladder. If the ladder is moving very fast, it appears shorter to someone watching from the garage. When the ladder is moving, the doors of the garage close for a short time when the ladder seems to fit inside. But if you were moving with the ladder, you would see that the doors did not close at the same time, so the ladder never really fit inside the garage all at once.

A Minkowski diagram can help show this. In the garage’s view, the ladder looks like it fits at one moment. But in the ladder’s view, it never fully fits inside the garage at the same time. This shows how motion changes what we see as happening at the same time.

Shutting the ladder in the garage

In a more complex version of the ladder paradox, we can trap the ladder inside a garage by closing both doors while it is moving inside. From the garage's view, once the ladder is fully inside and the doors are closed, the ladder stops and becomes longer than the garage, which would seem to cause a problem.

However, from the ladder's viewpoint, it was always longer than the garage. The key to understanding this is that the parts of the ladder stop moving one after another, starting from the front and moving to the back. This explains how the ladder ends up trapped inside the garage even though it appears longer from its own perspective.

This situation is similar to the twin paradox, where one twin travels at high speed and returns younger than the other. In both cases, the difference comes from the acceleration and deceleration involved in the journey.

Ladder paradox and transmission of force

Figure 9: A Minkowski diagram of the case where the ladder is stopped by impact with the back wall of the garage. The impact is event A. At impact, the garage frame sees the ladder as AB, but the ladder frame sees the ladder as AC. The ladder does not move out of the garage, so its front end now goes directly upward, through point E. The back of the ladder will not change its trajectory in spacetime until it feels the effects of the impact. The effect of the impact can propagate outward from A no faster than the speed of light, so the back of the ladder will never feel the effects of the impact until point F (note the 45° angle of the line A-F, corresponding to the speed of light transmission of information) or later, at which time the ladder is well within the garage in both frames. Note that when the diagram is drawn in the frame of the ladder, the speed of light is the same, but the ladder is longer, so it takes more time for the force to reach the back end; this gives enough time for the back of the ladder to move inside the garage.

If the back door of the garage is closed and will not open, the ladder will stop when it hits the door. This creates a puzzle: in the garage’s view, the ladder fits inside before hitting the door, but the ladder thinks it is too long to fit. The problem comes from thinking of the ladder as perfectly solid and unchanging shape. But special relativity says nothing can send information faster than light. So when the front of the ladder hits the door, the back of the ladder does not know yet and keeps moving forward. Only later, when the news of the collision catches up, does the back of the ladder slow down. Both ways of looking at it agree on what happens.

After the news reaches the back of the ladder, different things could happen — the ladder might bend or, at very high speeds, break apart. light cone

Man falling into grate variation

This version of the paradox was suggested by Wolfgang Rindler. It imagines a fast-walking person, shown as a rod, falling into a grate. From the grate’s view, the rod looks shorter and fits into the grate. But from the rod’s view, the grate looks shorter, making it seem like the rod is too long to fit.

The key idea is that the movement happening at the same time for the grate does not happen at the same time for the rod. In the rod’s view, the front starts moving down first, then the rest of the rod follows. This can make the rod seem bent in its own view. For this effect to be seen, both the rod and the grate need to be big enough for the time it takes to matter.

Main article: paradox

Bar and ring paradox

The bar and ring paradox is a simple idea from special relativity. Imagine a bar that is just a little longer than a ring. When the bar moves very fast upward and to the right, it looks shorter because of something called Lorentz contraction. At one moment, the bar looks short enough to fit through the ring.

But there is a puzzle. If we think from the bar’s point of view, the ring is moving. From this angle, the ring looks squashed, but the bar does not. How can the bar go through the ring? The answer is about what we mean by “at the same time.” When things move, what seems to happen at the same time can change. Because of this, the bar and ring do not line up perfectly all at once, which lets the bar pass through the ring even when it seems like it should not.

This article is a child-friendly adaptation of the Wikipedia article on Ladder paradox, available under CC BY-SA 4.0.

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