Spacetime diagrams can help you to visualize relativity. They are similar to scale diagrams and freebody diagrams.

Slides:



Advertisements
Similar presentations
Special Relativistic Paradoxes PHYS 206 – Spring 2014.
Advertisements

Space Fight.
O’ O X’ X Z’ Z 5. Consequences of the Lorentz transformation
Building Spacetime Diagrams PHYS 206 – Spring 2014.
Classical Relativity Galilean Transformations
 Today we will cover R4 with plenty of chance to ask questions on previous material.  The questions may be about problems.  Tomorrow will be a final.
Classical Doppler Shift Anyone who has watched auto racing on TV is aware of the Doppler shift. As a race car approaches the camera, the sound of its engine.
Wednesday, October 24: Midterm #1 Material covered: Events, reference frames, spacetime The interval Simultaneity (and relativity thereof) Lorentz transformations.
1 Special Relativity 2. 2 Topics l Recap l Length Contraction l Cosmic Ray Muons l Spacetime l Summary.
Space Fight Spacecraft of equal rest length pass very, very close to each other as they travel in opposite directions at a relative speed of 3/5 c. F.
Special Relativity. Clock A is at rest in our frame of reference and Clock B is moving at speed (3/5) c relative to us. Just as Clock B passes Clock A,
Chapter 36. Which of these is an inertial reference frames (or a very good approximation)? 1. A car rolling down a steep hill 2. A rocket being launched.
Conducted by: Adrian Lorenzana David Harris Muon Speed/Lifetime Study.
SPECIAL RELATIVITY -Postulates of Special Relativity -Relativity of time –> time dilation -Relativity of length –> length contraction © 2005.
Event P is shown by a small x. At what time (in the primed frame) does P occur? A] at ct’=1 B] at ct’=2 C] at ct’=3 D] at ct’=4.
Principle of special relativity Their is inconsistency between EM and Newtonian mechanics, as discussed earlier Einstein proposed SR to restore the inconsistency.
LECTURE # 4 DOPPLER –SPACETIME DIAGRAMS PHYS 420-SPRING 2006 Dennis Papadopoulos.
Life in the fast lane: the kinematics of Star Trek.
Special Relativity & General Relativity
Time Dilation, Length Contraction and Doppler
Life in the fast lane: the kinematics of Star Trek.
Lecture 14 Space-time diagrams (cont) ASTR 340 Fall 2006 Dennis Papadopoulos.
Special Relativity The Death of Newtonian Physics.
Copyright © 2010 Pearson Education, Inc. Lecture Outline Chapter 29 Physics, 4 th Edition James S. Walker.
IB Physics – Relativity Relativity Lesson 2 1.Time dilation 2.Lorentz Factor 3.Proper time 4.Lorentz contraction 5.Proper length 6.Twin paradox and symmetric.
A lecture series on Relativity Theory and Quantum Mechanics The Relativistic Quantum World University of Maastricht, Sept 24 – Oct 15, 2014 Marcel Merk.
You may pick up your R1 and R2 problems on the front desk. There are 5 points possible on each. The solutions are on-line, password is PH365. R3 problems.
Time Dilation and Lorentz Contraction Physics 11 Adv.
Muons are short-lived subatomic particles that can be produced in accelerators or when cosmic rays hit the upper atmosphere. A muon at rest has a lifetime.
Twin Paradox The Theory of Relativity. About Relativity As an object approaches the speed of light, time slows down. (Moving clocks are slow) (Moving.
Page 1 Phys Baski Relativity I Topic #9: Special Relativity I Transformation of Variables between Reference Frames –Non-relativistic Galilean Transformation.
Phy107 Fall From last time… Galilean Relativity –Laws of mechanics identical in all inertial ref. frames Einstein’s Relativity –All laws of physics.
Tue. Jan. 6 – Physics Lecture #17 Relativity – SpaceTime 1) Invariants & Spacetime interval 2) Time-like, Light-like, Space-like intervals 3) Spacetime.
Goal: To get to know the ins and outs of relativity (relatively speaking) Objectives: 1)To understand how Black holes compare to space-time 2)To learn.
Albert Einstein Born in 1879 died in 1955 Father of Modern Physics Relativity – describes the very large Quantum mechanics – describes the very small.
IB Physics 12 Mr. Jean January 7 th, The Plan: Video clip of the day Review of Time Dilation Length Contraction Space Time.
Physics 2170 – Spring Special relativity Homework solutions are on CULearn Remember problem solving sessions.
Education Physics Deparment UNS
Consequences of Lorentz Transformation. Bob’s reference frame: The distance measured by the spacecraft is shorter Sally’s reference frame: Sally Bob.
Physics 2170 – Spring Special relativity Homework solutions are on CULearn Remember problem solving sessions.
Einstein’s theory of special relativity makes some very bizarre and counter-intuitive predictions. Anything that violates common sense like this must.
Special Relativity I wonder, what would happen if I was travelling at the speed of light and looked in a mirror?
Einstein’s theory of special relativity makes some very bizarre and counter-intuitive predictions. Anything that violates common sense like this must.
Astronomy 1143 – Spring 2014 Lecture 18: Special Relativity.
My Chapter 26 Lecture.
The Twin Paradox Brenda goes off at 4/5 c to a distant star and then returns. Her twin brother Ali stays on Earth. When she gets back she is no longer.
1 Relativity  H3: Relativistic kinematics  Time dilation  Length contraction.
Special Relativity Physics 102: Lecture 28 Make sure your grade book entries are correct.
Special Relativity Physics 12 Adv. Einstein’s Postulates  In 1905, while working as a patent clerk in Switzerland, Einstein published his paper on.
1 PHYS 3313 – Section 001 Lecture #5 Wednesday, Sept. 11, 2013 Dr. Jaehoon Yu Time Dilation & Length Contraction Relativistic Velocity Addition Twin Paradox.
Visual Guide to Special and General Relativity. This is about to get weird…
1 1.Time Dilation 2.Length Contraction 3. Velocity transformation Einstein’s special relativity: consequences.
Time Dilation. Relative Time  Special relativity predicts that events seen as simultaneous by one observer are not simultaneous to an observer in motion.
Consequences of Relativism SPH4U. Wind Back the Clock Two consequences of relativism discussed: To a stationary observer, time appears to slow down in.
X’ =  (x – vt) y’ = y z’ = z t’ =  (t – vx/c 2 ) where   1/(1 - v 2 /c 2 ) 1/2 Lorentz Transformation Problem: A rocket is traveling in the positive.
Problem: A rocket travels away from earth at constant speed v to planet Q. The trip takes 100 years, as measured on earth but only 25 years as measured.
Some places where Special Relativity is needed
Special Relativity II Two-minute movie Quiz Breakdown of simultaneity
The Relativistic Quantum World
Quiz_09 Relativity – simultaneity, time dilation, length contraction
Problem: A rocket travels away from earth at constant speed v to planet Q. The trip takes 100 years, as measured on earth but only 25 years as measured.
Late 1800’s: Physics was triumphant!
Lorentz Transformation
Einstein’s Relativity Part 2
Given eqns Also P4.
The Cosmic Speed Limit Suppose you launch a pod at ½ c from a rocket traveling at ½ c relative to the Earth. How fast will it go?
Time Dilation Observer O is on the ground
Aim: How do we explain the special theory of relativity?
A rocket ship is heading toward you at ½ c
Presentation transcript:

Spacetime diagrams can help you to visualize relativity. They are similar to scale diagrams and freebody diagrams.

A spacetime diagram has time vertical. The axes are calibrated in years and light-years. t x

Which line represents an object at rest? t x ABCDABCD

Which line represents light? t x ABCDABCD

Which line represents an impossible motion? t x ABCDABCD t x Do question #1.

Draw a line for an object moving at 3/5 c. This will be the t’ axis for the ‘moving’ frame. t x t x

Which one is correct? x t’ t x x t x t x x A B C

A speed of 3/5 c has a slope of 5/3. x t’ t Rise = 5 Run = 3

Which is the correct x’ axis? x t’ t x x x’ t x t x t x A B C t’ x’

Hint: What is true about light in all frames? x t’ t x x x’ t x t x t x A B C t’ x’

x t’ t The speed of light is one light-year per year in all frames, so c =  x/  t. x’  run  x rise  t

x t’ t Similarly, c =  x’/  t’. x’  run  x’ rise  t’ Do question #2.

The Cosmic Speed Limit The cyclotron at TRIUMF can form charged pions moving at 0.96 c. These decay by emitting muons and neutrinos at high speeds. The emitted particles go faster than 0.96 c but they never go faster than c. Suppose you launch a pod at ½ c from a rocket traveling at ½ c relative to the Earth. How fast will it go?

x t’ t The pod travels at ½ c relative to the rocket. Which line is the pod’s? x’ ABCDABCD

x t’ t x’ The pod must cover one unit of space in two units of time. ABCDABCD

x t’ t How fast is it moving relative to the Earth? x’

x t’ t It travels at 4/5 c x’ Do question #3.

Time Slows Down You are in a rocket ship moving at 3/5 c past the Earth and send a signal to Earth every time your heart beats. Doctors on Earth say that your pulse is slow. If they sent a signal to you every time their heart beat, you would say that their heart was beating A) fast B) normal C) slow How is this possible?

x x’ This line marks all the places with simultaneous later times, t. The x axis marks all the places where t = 0. t’ t

x x’ The x’ axis marks all the points where t’ = 0. This line marks later simultaneous times, t’, in the other frame, F’. t’ t

What is , if the relative speed of the two frames is 3/5 c? x t’ t x’t”  = 1/ 1 – v 2 /c 2  = 5/4

x t’ t x’ What is t’, if t = 10? 108 Frame F sees time slowed in F’.

x t’ t x’ What is t, if t’ = 8? 10 8 Frame F’ sees time slowed in F. 6.4 Both frames can see each other’s time slowed because they disagree on simultaneity. There are three spacetime points, not two.

x t’ t x’ In what order do the three explosions happen? Which events(s) could the black explosion cause? If the black event caused another event then a signal had to travel at c, or a slower speed to the second event.

Muons are formed at the top of the atmosphere by cosmic rays and race toward the Earth at c. What is gamma at this speed?

The atmosphere is 10 km think. How long does it take for the muons to pass through the atmosphere? t = 10,000 m/0.995 x 3.00 x 10 8 m/s = 3.35 x s

The muons time has been slowed down. How much time passes for them? 3.3 x s/10 = 3.3 x s

The muons say that the time is shorter, but they agree on the speed of c. How is this possible? They say that the atmosphere is only 1 km thick. The atmosphere is moving relative to them and is contracted by gamma.

This a muon going at 3/5 c through the atmosphere. The muons measure a shorter time and they also measure a shorter atmosphere. t’ 10 t 8 x 8 x’

The muons measure the shortest time for any frame and this is called the ‘proper’ time. The Earth measures the longest distance and this is called the ‘proper’ distance t’ 10 t 8 x 8 x’