Physics HL
Physics HL
5
Chapters
329
Notes
Theme A - Space, Time & Motion
Theme A - Space, Time & Motion
Theme B - The Particulate Nature Of Matter
Theme B - The Particulate Nature Of Matter
Theme C - Wave Behaviour
Theme C - Wave Behaviour
Theme D - Fields
Theme D - Fields
Theme E - Nuclear & Quantum Physics
Theme E - Nuclear & Quantum Physics
IB Resources
Theme A - Space, Time & Motion
Physics HL
Physics HL

Theme A - Space, Time & Motion

Understanding Relativistic Velocity Addition: Lorentz vs. Galilean

Word Count Emoji
648 words
Reading Time Emoji
4 mins read
Updated at Emoji
Last edited on 5th Nov 2024

Table of content

Introduction 🚀

Relativity, as described by Einstein, challenges our everyday understanding of motion. Forget what you know about velocities simply adding up. Instead, we have to rely on some nifty equations. But don't panic! We've got spaceships, Jean and Phillipe, and even some math to help you out.

Velocity in different frames - basics

  • Galilean Relativity: This is your everyday, simple kind of relativity. In this view
  • If a spaceship moves at uA​ in frame A and frame B moves at v relative to frame A, then the spaceship's velocity in frame B is -uB ​= uA ​− v.
  • Einstein Relativity (Special Relativity): Things get spicy!
  • If our spaceship in frame A goes at the speed of light, and the observer in frame B sees it going the opposite way, the speed would look faster than light. That's a big NO-NO in Einstein's world.

Einstein's solution - lorentz equations

To make sense of these super-fast velocities, we use the Lorentz transformations: uB ​=\(u_B = \frac {x^I}{t^I} = \frac {γ(x - vt)}{γ{(t - vx / c^2)}}\)​ Where

  • ′x′ and ′t′ are the distance and time in frame B.
  • γ (gamma) is the Lorentz factor.

This leads to our superstar equation for relativistic velocity addition - 2uB​=1−c2uA​v​uA​−v​

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IB Resources
Theme A - Space, Time & Motion
Physics HL
Physics HL

Theme A - Space, Time & Motion

Understanding Relativistic Velocity Addition: Lorentz vs. Galilean

Word Count Emoji
648 words
Reading Time Emoji
4 mins read
Updated at Emoji
Last edited on 5th Nov 2024

Table of content

Introduction 🚀

Relativity, as described by Einstein, challenges our everyday understanding of motion. Forget what you know about velocities simply adding up. Instead, we have to rely on some nifty equations. But don't panic! We've got spaceships, Jean and Phillipe, and even some math to help you out.

Velocity in different frames - basics

  • Galilean Relativity: This is your everyday, simple kind of relativity. In this view
  • If a spaceship moves at uA​ in frame A and frame B moves at v relative to frame A, then the spaceship's velocity in frame B is -uB ​= uA ​− v.
  • Einstein Relativity (Special Relativity): Things get spicy!
  • If our spaceship in frame A goes at the speed of light, and the observer in frame B sees it going the opposite way, the speed would look faster than light. That's a big NO-NO in Einstein's world.

Einstein's solution - lorentz equations

To make sense of these super-fast velocities, we use the Lorentz transformations: uB ​=\(u_B = \frac {x^I}{t^I} = \frac {γ(x - vt)}{γ{(t - vx / c^2)}}\)​ Where

  • ′x′ and ′t′ are the distance and time in frame B.
  • γ (gamma) is the Lorentz factor.

This leads to our superstar equation for relativistic velocity addition - 2uB​=1−c2uA​v​uA​−v​

Unlock the Full Content! File Is Locked Emoji

Dive deeper and gain exclusive access to premium files of Physics HL. Subscribe now and get closer to that 45 🌟

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