Special Relativity Examples in Physics

Start with the recap, study the fully worked examples, then use the practice problems to check your understanding of Special Relativity.

This page combines explanation, solved examples, and follow-up practice so you can move from recognition to confident problem-solving in Physics.

Concept Recap

Special relativity is Einstein's theory describing physics at very high speeds, where measurements of time, length, and simultaneity depend on the observer's frame of reference.

At everyday speeds, classical physics works well. At speeds close to light, time and space behave differently from common intuition.

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How to Use These Examples

  • Read the first worked example with the solution open so the structure is clear.
  • Try the practice problems before revealing each solution.
  • Use the related concepts and background knowledge badges if you feel stuck.

What to Focus On

Core idea: Special Relativity asks whether the system is nuclear, quantum, or relativistic before using an everyday model.

Common stuck point: Students often know a formula related to special relativity but skip the recognition step: Does the situation involve particles, nuclei, photons, or relativistic speeds where everyday mechanics is not enough? That leads to a correct-looking substitution attached to the wrong physical model.

Sense of Study hint: Ask: Does the situation involve particles, nuclei, photons, or relativistic speeds where everyday mechanics is not enough?

Worked Examples

Example 1

medium
A rocket of proper length 100 m100\text{ m} passes Earth at v=0.6cv = 0.6c. What length does an Earth observer measure?

Answer

L=80 mL = 80\text{ m}

First step

1
Compute γ\gamma at v=0.6cv = 0.6c: γ=1/10.36=1.25\gamma = 1/\sqrt{1 - 0.36} = 1.25.

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Example 2

medium
A starship makes a round-trip to a star 4 ly4\text{ ly} away at v=0.8cv = 0.8c (Earth frame). How long does the trip take in Earth's frame, and how long aboard the ship?

Example 3

medium
A pion has proper lifetime 2.6×108 s2.6\times10^{-8}\text{ s}. In a lab it travels 39 m39\text{ m} before decaying. Roughly what was its γ\gamma? (Use vc=3.00×108 m/sv \approx c = 3.00\times10^8\text{ m/s}.)

Example 4

hard
Two spaceships approach each other, each moving at 0.6c0.6c relative to Earth. Find the speed of one as measured from the other.

Example 5

challenge
An electron is accelerated through a potential difference of 1.0 MV1.0\text{ MV}. Find γ\gamma and its final speed (rest energy 0.511 MeV0.511\text{ MeV}).

Practice Problems

Try these problems on your own first, then open the solution to compare your method.

Example 1

easy
Find the Lorentz factor γ\gamma for an object moving at v=0.6cv = 0.6c.

Example 2

easy
At everyday speeds (far below cc), is the Lorentz factor close to 11 or much larger?

Example 3

easy
A clock moving at high speed runs slow as seen by a stationary observer. What is this effect called?

Example 4

easy
A moving object appears shortened along its direction of motion. What is this called?

Example 5

easy
Find the rest energy of a 2 kg2 \text{ kg} object using E=mc2E = mc^2 (c=3×108c = 3\times10^8).

Example 6

easy
Should you use relativity formulas for a car moving at 30 m/s30 \text{ m/s}?

Example 7

easy
Find γ\gamma for v=0.8cv = 0.8c.

Example 8

easy
Does 'everything is relative' in physics relativity mean any opinion is as valid as another?

Example 9

medium
A muon's proper lifetime is 2×106 s2\times10^{-6} \text{ s}. At γ=5\gamma = 5, find its lifetime in the lab frame.

Example 10

medium
A rod has proper length 2 m2 \text{ m}. Moving at γ=2\gamma = 2, find its contracted length.

Example 11

medium
Find the energy equivalent of 0.5 kg0.5 \text{ kg} converted entirely to energy (c=3×108c = 3\times10^8).

Example 12

medium
At what speed (as a fraction of cc) does γ=2\gamma = 2?

Example 13

medium
A spaceship travels 0.6c0.6c. Its clock measures a 4 year4 \text{ year} trip. How long does an Earth observer measure? (γ=1.25\gamma = 1.25)

Example 14

medium
Find γ\gamma for v=0.99cv = 0.99c.

Example 15

medium
A particle's total relativistic energy is E=γmc2E = \gamma m c^2. For γ=3\gamma = 3, m=1×1027 kgm = 1\times10^{-27} \text{ kg}, find EE (c=3×108c = 3\times10^8).

Example 16

medium
A clock on a fast ship measures 3exthours3 ext{ hours} for a trip. With γ=2\gamma = 2, how long does a stationary observer measure?

Example 17

medium
A spaceship of proper length 30extm30 ext{ m} moves at γ=1.5\gamma = 1.5. Find its contracted length.

Example 18

challenge
A muon (γ=10\gamma = 10, proper lifetime 2.2×106 s2.2\times10^{-6} \text{ s}) moves at nearly cc. Find the distance it travels in the lab frame (c=3×108c = 3\times10^8).

Example 19

challenge
Find the kinetic energy of a particle with γ=2\gamma = 2, m=9.1×1031 kgm = 9.1\times10^{-31} \text{ kg} using KE=(γ1)mc2KE = (\gamma - 1)mc^2 (c=3×108c = 3\times10^8).

Example 20

challenge
Two events are simultaneous in one frame but not in another moving frame. What principle does this illustrate?

Example 21

easy
What is the Lorentz factor γ\gamma when v=0v = 0?

Example 22

easy
Find the Lorentz factor for v=0.5cv = 0.5c.

Example 23

easy
An electron has mass m=9.11×1031 kgm = 9.11 \times 10^{-31}\text{ kg}. Find its rest energy in joules. Use c=3.00×108 m/sc = 3.00 \times 10^8\text{ m/s}.

Example 24

easy
Find the Lorentz factor for v=0.95cv = 0.95c.

Example 25

easy
A spaceship moves at v=0.6cv = 0.6c. Its onboard clock ticks 1 s1\text{ s} per tick. How long is one tick as measured on Earth? (γ=1.25\gamma = 1.25)

Example 26

medium
A particle has rest mass m=1.67×1027 kgm = 1.67\times10^{-27}\text{ kg} (a proton). Find its total energy at γ=4\gamma = 4. Use c=3.00×108 m/sc = 3.00\times10^8\text{ m/s}.

Example 27

medium
At what speed (as a fraction of cc) does the Lorentz factor equal γ=1.25\gamma = 1.25?

Example 28

medium
A muon's proper lifetime is 2.2×106 s2.2\times10^{-6}\text{ s}. At v=0.99cv = 0.99c (γ7.09\gamma \approx 7.09), find its lifetime in the lab frame.

Example 29

medium
Find the Lorentz factor for v=0.9cv = 0.9c.

Example 30

medium
Find the kinetic energy of an electron (m=9.11×1031 kgm = 9.11\times10^{-31}\text{ kg}) at γ=3\gamma = 3. Use c=3.00×108 m/sc = 3.00\times10^8\text{ m/s}.

Example 31

medium
A spaceship of proper length 60 m60\text{ m} is measured to be 30 m30\text{ m} long by an Earth observer. Find γ\gamma.

Example 32

medium
Find the relativistic momentum of a proton (m=1.67×1027 kgm = 1.67\times10^{-27}\text{ kg}) at v=0.6cv = 0.6c. Use c=3.00×108 m/sc = 3.00\times10^8\text{ m/s}.

Example 33

medium
Convert 0.511 MeV0.511\text{ MeV} to joules. (1 eV=1.6×1019 J1\text{ eV} = 1.6\times10^{-19}\text{ J}.)

Example 34

hard
A particle is accelerated until its total energy is 55 times its rest energy. Find its speed as a fraction of cc.

Example 35

hard
A spaceship moves at 0.8c0.8c relative to Earth and launches a probe forward at 0.5c0.5c relative to itself. Find the probe's speed relative to Earth.

Example 36

hard
An electron has total energy E=1.022 MeVE = 1.022\text{ MeV}. Find its kinetic energy in MeV\text{MeV}.

Example 37

hard
A particle has rest energy 938 MeV938\text{ MeV} (a proton) and kinetic energy 2814 MeV2814\text{ MeV}. Find γ\gamma.

Example 38

hard
A photon has energy EE. Find its momentum.

Example 39

hard
A clock on a satellite runs at γ=1+5×1011\gamma = 1 + 5\times10^{-11} slower than ground clocks. Roughly how many extra nanoseconds does the satellite clock lose per day relative to ground (consider only this γ\gamma effect)?

Example 40

challenge
A particle has momentum p=3mcp = 3mc. Find its total energy in units of mc2mc^2.

Example 41

challenge
In frame SS, two events at x1=0x_1 = 0 and x2=600 mx_2 = 600\text{ m} are simultaneous. In frame SS' moving at v=0.6cv = 0.6c along +x+x, what is the time difference Δt\Delta t' between the events? Use c=3×108 m/sc = 3\times10^8\text{ m/s}.

Background Knowledge

These ideas may be useful before you work through the harder examples.

speed of lightreference frame