2.3.30 · D1Modern Physics

Foundations — Length contraction — derivation

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This page assumes nothing. Before you touch the derivation in the parent note, every letter and every symbol it throws at you is unpacked here — meaning first, picture second, purpose third. Read it top to bottom; each block leans on the one above it.


0. What is a "frame"? (the ground everything stands on)

Before any symbol, we need the idea of a reference frame.

The whole topic is a conversation between two frames, so we give each a name:

  • — the ground / lab frame. Picture you standing still on a platform. In this frame the rod goes whizzing past.
  • — the rod's own frame. Picture yourself sitting on the rod, riding along with it. In this frame the rod is perfectly still and the ground rushes past instead.

The little tick mark in (read "S-prime") just means "the second observer's stuff." Positions measured by that observer get a prime too: , .

Figure — Length contraction — derivation

Prime :::- means "belongs to the second observer " — it does not mean a derivative here.


1. Position and time — the two things we ever record

Picture a single dot on a strip: its horizontal spot is , and stamped next to it is the time it was there.

Why the topic needs it: to talk about "where the front end is when," you need both a place and a moment. That "place-and-moment" bundle is exactly an event, and length contraction is built entirely out of comparing events.


2. Speed and the speed of light

is a pure number between :::- and — it has no units, and it measures "what fraction of light speed."


3. The Lorentz factor — the master dial

Everything in this topic is scaled by one number. Meet it slowly.

Let's build it from the inside out so no piece is mysterious:

  • — square the speed-fraction. Since is between and , this is also between and .
  • — subtract from one. At rest () this is ; near light-speed it shrinks toward .
  • — take the square root, still between and .
  • — flip it. Dividing by a small number gives a big number.
Figure — Length contraction — derivation

Look at the curve above. It is flat and boring near (everyday life — , relativity invisible), then rockets upward as . This shape is why you never notice contraction in a car but must account for it in a particle accelerator.

Why the topic needs it: the final formula is . Because , dividing by it can only make things smaller or equal — that single inequality is "contraction." See Lorentz factor gamma for the deep dive.

At , what is ? :::- (frames agree, no contraction). As , what happens to ? :::- It grows without bound, .


4. Proper length vs measured length

Now the two starring quantities.

Figure — Length contraction — derivation

The subscript in means :::- "measured in the rest frame" (the proper value), not "at time zero."


5. Simultaneity — the secret engine

This is the concept the parent note leans on hardest, so we picture it carefully.

Here is the twist that makes relativity relativity:

Figure — Length contraction — derivation

Why the topic needs it: in the derivation, setting in frame is the single step that makes the terms cancel. Without simultaneity, there is no contraction — it is the engine, not a footnote.


6. The Lorentz transformation — the dictionary between frames

The parent note starts from one equation. Here is what it says.

Read the right-hand side in plain words:

  • — "start from where the event is in , then slide back by how far the rod-frame has travelled ()." This is the ordinary, common-sense part (it's what you'd write even without relativity).
  • — multiply the whole thing by . This is the purely relativistic correction: the stretch that accounts for the frames' disagreeing rulers.

Without the factor , the transformation would :::- be the old (Galilean) rule that wrongly assumes a shared universal clock.


Prerequisite map

Speed of light c is the same for all

Lorentz transformation x'=gamma x-vt

Relative speed v

Lorentz factor gamma

Two frames S and S-prime

Events place x and time t

Simultaneity t1 equals t2

Length needs both ends at one instant

Length contraction derivation

Proper length L0 rest frame

Measured length L moving frame

L equals L0 over gamma


Equipment checklist

Cover the right side and see if you can answer each before revealing.

What is a reference frame?
An observer together with their rulers and clocks — one consistent point of view for measuring where and when.
What do and stand for here?
= ground/lab frame (rod moves); = rod's own rest frame (rod still, ground moves).
What is an "event"?
A place and a time together, a pair .
Why do we always write speeds as a fraction of ?
Because only the ratio matters; is the universal yardstick for "how fast is fast."
Write the Lorentz factor and its value at .
; at , .
Is ever less than 1?
No — always, and equals only when .
What does the subscript in mean?
"Rest frame / proper," i.e. measured where the object is stationary — not time zero.
Which is larger, or ?
The proper length ; the moving-frame is smaller (or equal).
What makes two events "simultaneous"?
They share the same time reading, , in that frame.
Why must a length measurement use simultaneous endpoint marks?
Because a moving rod slides; marking the ends at different times gives its length plus the distance it drifted — garbage.
What does the Lorentz transformation do?
Translates an event's ground-frame position/time into its position in the rod's rest frame.
Why isn't plain enough?
That old rule assumes one universal clock; the factor is the correction that keeps the same for everyone.

Connections

  • Length contraction — derivation — the parent this page prepares you for.
  • Lorentz transformation — the dictionary between frames, used in every step.
  • Lorentz factor gamma — the master dial built here.
  • Relativity of simultaneity — the engine behind the effect.
  • Time dilation — the opposite twin ().
  • Spacetime interval — where the square root in comes from.
  • Muon decay experiment — the real-world payoff.