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F. Revolutions in Modern Physics: Quantum Mechanics and Special Relativity · Special Relativity

Einstein's Two Postulates and the Power of Thought Experiments

F1.1 F2.1 F3About 65 minutes
Learning goals
  • I can state Einstein's two postulates of special relativity.
  • I can explain how Einstein used thought experiments to reach his postulates.
  • I can apply the postulates to predict what different inertial observers measure for the speed of light.
  • I can describe evidence that the speed of light does not depend on the motion of its source or the observer.

Words to know

postulate
A basic statement accepted as true without proof, from which a theory is built. A postulate is tested by checking its consequences against experiments.
special relativity
Einstein's 1905 theory of space and time for observers in inertial frames, built on two postulates.
principle of relativity (Einstein)
Postulate 1: all the laws of physics, including electromagnetism and optics, are the same in every inertial frame.
constancy of the speed of light
Postulate 2: light in a vacuum travels at the same speed c = 3.00 × 10⁸ m/s in every inertial frame, whatever the motion of the source or observer.
thought experiment
An experiment carried out in the imagination, following the laws of physics carefully, to explore the consequences of a theory (German: Gedankenexperiment).
invariant
A quantity that has the same value in every inertial frame. In special relativity, c is invariant.

A teenager chases a light beam

Einstein later wrote that, at about age 16, he wondered what he would see if he could run alongside a beam of light at speed c. The wave would look frozen: electric and magnetic fields varying in space but not changing in time. Yet Maxwell's equations allow no such thing. A frozen light wave is impossible.

So either Maxwell's equations fail for a fast-moving observer, or no observer can ever catch up to light. Ten years later, Einstein built a theory on the second answer. He did it mostly in his head, with thought experiments: imagined situations worked out carefully using physical laws. This lesson is about the two simple statements at the heart of that theory, and why they were so radical.

The magnet and the conductor

Einstein's 1905 paper "On the Electrodynamics of Moving Bodies" opens with another thought experiment. Move a magnet toward a coil of wire and a current flows. Move the coil toward the magnet instead, at the same relative speed, and exactly the same current flows. Yet the physics of the time explained the two cases differently: in one, a changing magnetic field creates an electric field; in the other, the magnetic force acts on moving charges in the wire.

To Einstein, giving two different explanations for one observed result was a sign that something was wrong. Only the relative motion of the magnet and coil seemed to matter. That suggested the principle of relativity should apply to electricity and magnetism too, not just to mechanics.

Frame 1: coil at restSNmagnet movescoilchanging magnetic field→ induced currentFrame 2: magnet at restSNcoil movesmagnetic force on movingcharges → the same currentSame relative motion, same current: only relative motion matters.
Einstein's magnet-and-conductor thought experiment. Whether the magnet moves or the coil moves, the same induced current flows. Only relative motion matters, which suggests the principle of relativity holds for electromagnetism as well as mechanics.

The two postulates (1905)

Postulate 1, the principle of relativity: The laws of physics are the same in all inertial frames of reference.

Postulate 2, the constancy of the speed of light: Light in a vacuum travels at the same speed, c = 3.00 × 10⁸ m/s, in every inertial frame, regardless of the motion of the source or of the observer.

Postulate 1 extends Galileo's principle from mechanics to all of physics, including Maxwell's equations. Postulate 2 follows from it: if Maxwell's equations hold in every inertial frame, then every inertial observer must measure light at the speed c those equations predict.

Each statement sounds harmless. Together they are explosive, because they contradict the Galilean velocity rule u = u′ + v. If a spacecraft moving at 0.60c sends a light pulse forward, Galileo says Earth measures 1.60c. Einstein says Earth measures c, and so does the crew. Both cannot be right.

Galilean prediction (wrong)0.60clightEarth measures c + 0.60c = 1.60cWhat is actually measured (Einstein)0.60clightEarth measures exactly c
A spacecraft moving at 0.60c relative to Earth sends a light pulse forward. Galilean addition predicts 1.60c. By Einstein's second postulate, Earth observers and the crew both measure exactly c.

What has to give?

Speed is distance divided by time. If two observers moving relative to each other measure the same speed for the same light pulse, then they must disagree about distances, about times, or both. Einstein realized that Newton's assumptions of absolute space and absolute time had never been tested at speeds near c. He dropped them. The consequences fill the rest of this unit:

  • Simultaneity is relative: two events at the same time for one observer can happen at different times for another (lesson 4).
  • Moving clocks run slow: time dilation (lesson 5).
  • Moving objects are shorter: length contraction (lesson 7).
  • Velocities do not simply add, and nothing with mass reaches c (lessons 9 and 10).
  • Mass is a form of energy: E = mc² (lesson 11).

And the ether? With postulate 2, light needs no special frame, so the ether is unnecessary. Einstein wrote that introducing a 'light ether' would prove superfluous.

Evidence that c is the same for everyone

  • Michelson–Morley (1887) and its many repeats: no difference in light speed along different directions as Earth moves (lesson 2).
  • Double stars: in 1913 Willem de Sitter argued that if light from an approaching star moved faster than light from a receding one, the images of orbiting double stars would be badly scrambled. Their orbits look regular, so light's speed does not depend on the speed of its source.
  • Fast-moving sources: in 1964 at CERN, physicists timed gamma rays given off by neutral pions travelling at more than 0.999c. Galileo would predict nearly 2c. The gamma rays travelled at c.

Today the second postulate is built into the definition of the metre: since 1983, the metre has been defined as the distance light travels in a vacuum in 1/299 792 458 of a second, so c is exactly 299 792 458 m/s.

Worked example

Example 1: Applying the second postulate

A spacecraft moves away from Earth at 0.80c and fires a laser pulse backward toward Earth. (a) What speed does the crew measure for the pulse? (b) What speed does an Earth observer measure? (c) What would Galilean addition predict for (b)?

  1. (a) Postulate 2: every inertial observer measures light in vacuum at c. The crew measures c.
  2. (b) Earth is also an inertial frame, so Earth measures c as well.
  3. (c) Galilean: u = u′ + v. Toward Earth is negative for u′: u = −c + 0.80c = −0.20c, a speed of 0.20c. This is not what happens.

(a) c; (b) c; (c) 0.20c (wrong). The source's motion does not change the speed of light.

Worked example

Example 2: Can you tell you are moving?

You wake up in a windowless spacecraft. The engines are off and nothing pushes you. Can any experiment inside the ship (a pendulum, a magnet and coil, a measurement of the speed of light) tell you your speed?

  1. With the engines off and no forces, the ship is an inertial frame.
  2. Postulate 1: all the laws of physics are the same in every inertial frame. Every experiment gives the same result as in any other inertial frame.
  3. Postulate 2: even measuring light speed in different directions gives c every time, so light cannot reveal your motion either.

No. No experiment inside an inertial frame can measure 'absolute' velocity. Only motion relative to other objects (for example, a star seen through a window) can be measured.

Worked example

Example 3: Distance or time must change

A light pulse is sent from the front of a train to the back. The train is 300 m long in its own frame. (a) How long does the trip take in the train's frame? (b) A ground observer sees the train moving forward, so the back of the train is moving toward the pulse. Explain, using postulate 2, why the ground observer cannot measure the same time unless distances or times differ between frames.

  1. (a) t′ = L/c = 300 m ÷ 3.00 × 10⁸ m/s = 1.00 × 10⁻⁶ s = 1.00 µs.
  2. (b) For the ground observer, the pulse still moves at c, but the back of the train moves toward it, so the pulse covers less distance than the train's length before meeting it.
  3. Same speed, different distance: the ground observer must measure a different time (unless the train's length is also different). Either way, at least one of distance and time is not absolute.

(a) 1.00 µs. (b) With light speed fixed at c for both, the two observers cannot agree on both the distance and the time. That is the doorway to the relativity of simultaneity, time dilation and length contraction.

Postulates and evidence

A postulate is not 'just a guess'. It is a starting point whose consequences can be tested. Special relativity has passed every test for more than a century: particle accelerators, atomic clocks and GPS all confirm its predictions every day.

Just for fun

Einstein's 1905 relativity paper contains no references to anyone else's papers at all. Its only acknowledgement thanks his friend and patent-office colleague Michele Besso for helpful discussions.

Hands-on activity

Measure the speed of light with a microwave oven

Postulate 2 says c is the same for everyone. You can measure it in your kitchen!

You need: a microwave oven, a microwave-safe plate, a chocolate bar (or a few slices of cheese, or marshmallows spread in one layer), a ruler. Safety: an adult must help. Never run a microwave empty. Melted food is hot.

  1. Remove the turntable (ask an adult how; on some ovens it lifts out; on others place an upside-down microwave-safe bowl over the spindle and set the plate on that so it does not turn).
  2. Lay the chocolate flat on the plate. Microwave on high for 15 to 20 seconds only, until a few spots just begin to melt.
  3. Microwaves inside the oven form standing waves. The melted spots are at the antinodes, where heating is strongest. Measure the distance d between the centres of two neighbouring melted spots in cm.
  4. Neighbouring antinodes are half a wavelength apart, so λ = 2d. Look on the label inside the door or on the back of the oven for the frequency f (most ovens use 2450 MHz = 2.45 × 10⁹ Hz).
  5. Calculate c = fλ = f × 2d. Compare with 3.00 × 10⁸ m/s and find your percentage difference.

What to look for: spots about 6 cm apart. With d = 6.1 cm, λ = 0.122 m and c = (2.45 × 10⁹)(0.122) ≈ 3.0 × 10⁸ m/s. Uneven melting and the difficulty of finding a spot's centre usually give 5 to 15% error. Then eat the data.

Your turn

1

State Einstein's two postulates.

2

Describe Einstein's 'chasing a light beam' thought experiment and the conclusion he drew.

3

A rocket moving toward a star at 0.50c receives light from the star. What speed does the crew measure for the light?

4

How does postulate 1 differ from Galileo's principle of relativity?

5

Why did Einstein say the ether was unnecessary?

6

Give two pieces of experimental evidence that the speed of light does not depend on the motion of its source.

7

Is a 'postulate' the same as a proven fact? Explain.

More practice: warm-up

1

What is the speed of light in a vacuum, to three significant figures?

2

In what year did Einstein publish special relativity?

3

What is a thought experiment?

4

Which classical assumptions did Einstein give up?

5

Does special relativity apply to accelerating frames?

More practice: on your own

1

A spaceship moving at 0.30c relative to Earth fires a light pulse forward and an identical pulse backward. What speeds do (a) the crew and (b) Earth observers measure? (c) What would Galilean physics predict for Earth?

2

Explain the magnet-and-conductor problem that bothered Einstein.

3

Why does postulate 1 lead directly to postulate 2?

4

A pulse of light takes 2.50 µs to travel the length of a laboratory in the lab's frame. How long is the lab?

5

The metre is defined from the speed of light. Explain why this definition only makes sense if postulate 2 is true.

Challenge

1

A spaceship moves at 0.60c past Earth. When it passes, it sends a light pulse forward toward a space station that is 1.80 × 10¹¹ m ahead (measured in Earth's frame, station at rest relative to Earth). (a) How long does the light take in Earth's frame? (b) In Earth's frame, how far ahead of the ship is the pulse at that instant? (c) Why don't the crew and Earth agree on how far ahead the pulse is after a given time, even though both say the pulse moves at c?

2

A friend says: 'Relativity says everything is relative, so the speed of light must be relative too.' Correct this statement.

3

Assess the role of thought experiments in the development of special relativity. Give two examples and explain one limitation.

Check your understanding

Quiz

1.

Which is Einstein's second postulate?

2.

A spaceship moving at 0.90c toward Earth turns on a headlight. What speed does an Earth observer measure for the light?

3.

What did Einstein conclude from imagining himself chasing a light beam?

4.

How does Einstein's first postulate extend Galileo's principle?

5.

Which observation supports the idea that light's speed does not depend on its source's speed?

6.

If two observers in relative motion measure the same speed for a light pulse, what must be true?

For parents and teachers

Big idea (F1.1, F2.1, F3): special relativity rests on two short statements: the laws of physics are the same in every inertial frame, and light always travels at c. Everything else in this unit follows from them. Einstein reached them largely through thought experiments.

How to help: Ask your teen to state the two postulates from memory and give one piece of evidence for the second one. The microwave activity needs an adult: the turntable must be removed or blocked, the oven must never run empty, and melted food is hot.

Common difficulties:

  • Thinking 'relativity' means 'everything is relative'. The laws of physics and the speed of light are the same for everyone.
  • Applying the Galilean rule u = u′ + v to light out of habit.
  • Treating a postulate as an unproven guess. Its predictions have been tested countless times.
  • Forgetting that the postulates are stated for inertial frames.