Special Relativity I wonder, what would happen if I was travelling at the speed of light and looked in a mirror?

Slides:



Advertisements
Similar presentations
Lecture 20 Relativistic Effects Chapter Outline Relativity of Time Time Dilation Length Contraction Relativistic Momentum and Addition of Velocities.
Advertisements

Classical Relativity Galilean Transformations
Physics Lecture Resources
Caroline Chisholm College
relativity Quantum Classic physics Modern physics.
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.
P1X*Dynamics & Relativity : Newton & Einstein Chris Parkes October 2005 Special Relativity Postulates Time Dilation Length Contraction Lorentz Transformation.
Cutnell/Johnson Physics 7th edition
Special and General Relativity
 PROGRAM OF “PHYSICS2B” Lecturer: Dr. DO Xuan Hoi Room A1. 413
1 Special Relativity (Ch 37) Modern physics special relativity quantum mechanics Both were developed to explain the “few remaining puzzles” of classical.
SPECIAL RELATIVITY -Postulates of Special Relativity -Relativity of time –> time dilation -Relativity of length –> length contraction © 2005.
Special Relativity & General Relativity
Chapter 37 Special Relativity. 37.2: The postulates: The Michelson-Morley experiment Validity of Maxwell’s equations.
Introduction to special relativity
S-164 Countdown G minus 15 and counting. Relativity AP Physics Supplemental.
Page 1 Phys Baski Relativity I Topic #9: Special Relativity I Transformation of Variables between Reference Frames –Non-relativistic Galilean Transformation.
Special relativity.
Special Theory of Relativity Space and Time. Inertial reference frames Reference frames in which Newton’s first law is valid. –In other words, a reference.
The Special Theory of Relativity. Galilean-Newtonian Relativity Definition of an inertial reference frame: One in which Newton’s first law is valid Earth.
Special Relativity: Time Dilation and Length Contraction SPH4U.
Special Relativity Einstein messes with space and time.
Relativity Introduction 14.1 Introduction Electrons can be accelerated to 0.99c using a potential difference of 3.1 MV According to Newtonian Mechanics,
Chapter 9 Relativity Basic Problems The formulation of Newtonian mechanics is based on our daily experience and observation. But, Newtonian mechanics.
USC2001 Energy Lecture 4 Special Relativity Wayne M. Lawton Department of Mathematics National University of Singapore 2 Science Drive 2 Singapore
The Theory of Special Relativity Ch 26. Two Theories of Relativity Special Relativity (1905) –Inertial Reference frames only –Time dilation –Length Contraction.
Time Dilation We can illustrate the fact that observers in different inertial frames may measure different time intervals between a pair of events by considering.
Consequences of Lorentz Transformation. Bob’s reference frame: The distance measured by the spacecraft is shorter Sally’s reference frame: Sally Bob.
Chapter 28: Special Relativity
Lecture_06: Outline Special Theory of Relativity  Principles of relativity: length contraction, Lorentz transformations, relativistic velocity  Relativistic.
Introduction to special relativity
Astronomy 1143 – Spring 2014 Lecture 18: Special Relativity.
My Chapter 26 Lecture.
Physics 12 MODERN PHYSICS: AN INTRODUCTION.  QUOTE AND CLIP OF.
Introduction Classical Physics Laws: Mechanics (Newton), Electromagnetism (Maxwell), Optics, Fluids,.. Etc. Modern Physics: What do we mean? Are the laws.
Special Relativity 1. Quiz 1.22 (10 minutes) and a few comments on quiz So far we know that Special Relativity is valid for all speeds. But it is.
Chapter 26 Relativity. General Physics Relative Motion (Galilean Relativity) Chapter 3 Section 5
IB Physics – Relativity Relativity Lesson 1 1.Galilean Transformations (one frame moving relative to another) Michelson Morley experiment– ether. 2.Speed.
1 Relativity  H3: Relativistic kinematics  Time dilation  Length contraction.
Special Relativity Additional reading: Higher Physics for CfE, p.64 – 69. Notes p.38 The idea of relativity goes back a long way … Gallileo was one of.
Unit 13 Relativity.
Consequences of Special Relativity Simultaneity: Newton’s mechanics ”a universal time scale exists that is the same for all observers” Einstein: “No universal.
Special Relativity Physics 102: Lecture 28 Make sure your grade book entries are correct.
Special Relativity Physics 12. Key Terms Postulate: a thing suggested or assumed to be true as the basis for reasoning, discussion, or belief Inertial.
Chapter 39 Relativity. A Brief Overview of Modern Physics 20 th Century revolution 1900 Max Planck Basic ideas leading to Quantum theory 1905 Einstein.
RELATIVITY IN EVERY INERITAL REFERENCE FRAME, THE SPEED OF LIGHT IS A CONSTANT BUT WHAT DOES THIS MEAN?
Visual Guide to Special and General Relativity. This is about to get weird…
Special Theory of Relativity. Galilean-Newtonian Relativity.
1 1.Time Dilation 2.Length Contraction 3. Velocity transformation Einstein’s special relativity: consequences.
Unit 1B: Special Relativity Motion through space is related to motion in time.
Galileo’s Relativity: Text: The laws of mechanics are the same in all inertial reference frames. More general: The laws of mechanics are the same in all.
Relativity made simple?. Newton Maxwell The Laws of Physics – the same in all “inertial” frames.
By: Jennifer Doran. What was Known in 1900 Newton’s laws of motion Maxwell’s laws of electromagnetism.
Special Relativity (Math)  Reference from Tipler chapter 39-1 to 39-3  Newtonian relativity  Einstein’s postulates  Lorentz transformation  Time dilation.
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.
Quiz: True or False 1.Length and time are absolute. 2.If we only had the technology, spaceships could theoretically travel at twice speed of light. 3.You.
Special Relativity and Time Dilation
Einstein’s Universe Dr Martin Hendry Dept of Physics and Astronomy,
Special Relativity Physics 102: Lecture 28
Classical Physics “Inertial Reference Frame” (Section 5.2):
Einstein’s Relativity Part 2
18.3 Special Relativity 1.
Unit 9: Special Relativity Lesson 1: The Theory
An Introduction To ‘High Speed’ Physics
RELATIVITY III SPECIAL THEORY OF RELATIVITY
Spacetime Structure.
Key Areas covered The speed of light in a vacuum is the same for all observers. The constancy of the speed of light led Einstein to postulate that measurements.
Physics 1161: PreLecture 26 Special Relativity 1.
space traveller is younger when they return v = 0 v = 0.87c v = 0.995c v = 0.999c v = c (?)
Chapter 37 Special Relativity
Presentation transcript:

Special Relativity I wonder, what would happen if I was travelling at the speed of light and looked in a mirror?

Gallileo laws of physics should be the same in all inertial frames of reference. ( moving at constant velocity ) Galilean Ivariance If you were on a bus moving at constant speed you would experience the laws in the same way as if you were at rest

Newton Introduced the idea of universal time and space. He believed that it was the same time at all points in the universe as it was on Earth, clocks tick at the same rate regardless of their movement. Clocks tick at the same rate relative to observers who may have a different motion to the clock.

Absolute Space A static background against which all movement can be referenced A train moving out of a station : which moves ? The station or the train ? Newton said that the train moved BUT is the station stationary ?

Galilean Transformations Train moves at 50 ms -1 to the left I walk at 5 m s -1 to the front / back of the train. What is my velocity relative to a stationary observer ?

Galilean Transformations 2 What about my velocity relative to someone stationary on the train ?

Galilean Transformations 3 Runner A, 5 ms -1, is moving left towards runner B, 10 ms -1 to the right. What is the velocity of runner A relative to runner B ?

Some language The train ( or lab or …. ) is called a ‘frame of reference’ The frame of reference is called an ‘inertial frame of reference’ when the movement is constant velocity

James Clerk Maxwell Light is an electromagnetic wave Predicted the speed of light to be 3.0x10 8 ms -1 If light is a wave,then is it passing through something ? Something must be vibrating. This was called the ether. Michelson and Morley set out to detect the motion of the earth through the ether ! No difference in speed of light as earth moves in different directions.

Einstein Speed of light is constant for all observers The laws of Physics are the same for all observers in all parts of the universe Leads to a new theory of motion : A spaceship travelling at 2.9 x 10 6 ms -1 approaches a stationary planet, it sends out a light signal to the planet. What speed does the observer on the planet measure the light to be travelling at ? If speed = distance / time and speed = frequency x wavelength then if the speed is to remain constant ‘ something’ must happen to the distance and time

Time Dilation Consider a person on a platform who shines a laser pulse upwards, reflecting the light off a mirror. The time interval for the pulse to travel up and down is t Travellers in this different frame of reference observe the ‘event’ (eg out of the window of the train), which takes place in the platform frame of reference and measure a time t’. platform mirror h Person in same frame as ‘event’ measures a time t. Total distance travelled by pulse 2h = ct. h v Person in same frame as event measures a time, t, Total distance travelled by pulse 2h = ct Travellers in this different frame of reference observe the ‘event’ (eg out of the window of the train), which takes place in the platform frame of reference and measure a time t’.

Time Dilation 2 Both observers measure the same speed for the speed of light Distance = 2h = ct Train frame of reference Horizontal distance travelled by train = vt’ Total distance travelled by pulse = ct’ Platform frame of reference

Time dilation 3 For the Train frame of reference: Draw a right angled triangle where the vertical side is height of pulse, ( 0.5ct), the horizontal side is half the distance, d, travelled by the train, 0.5 vt’ and the hypoteneuse is half he distance gone by the pulse as seen by travellers on the train( 0.5ct’ ). 0.5ct’ 0.5ct 0.5 vt’

Time Dilation 4 Apply Pythagorus (½ct) 2 + (½vt’) 2 = (½ct’) 2 (ct) 2 + (vt’) 2 = (ct’) 2 (ct) 2 = (ct’) 2 –(vt’) 2 c 2 t 2 = (t’) 2 (c 2 – v 2 )

Time Dilation 5 v = speed of train c = speed of light t = time for event as viewed by observer on platform ( stationary ) t’ = time for event as viewed by observer on train ( moving observer) Assumptions 1)Two frames are moving relative to each other along the x axis 2)Two observers on train as start / finish points are different.

Time Dilation 6 Example Dr Who is moving at a constant 0.92c., relative to earth. He measures the time between ticks,∆t, of his clock to be 1.0 s. What is ∆t measured as at on earth by Sarah Jane ? t = 1.0 s V = 0.92c. t’ = ? = 2.6 s From the point of view of the earth based observer ( Sarah Jane ),Dr Who’s clock runs slow.

Time Dilation 7 The term is called the gamma factor. At everyday speeds it is almost unity ( 1 ). For time dilation to be noticeable then ‘relative speed’ must be c.a. 10 % of c.

Length Contraction Consider a rod placed on the platform discussed previously. To measure the length :Fix a mirror to one end and fire a beam of light from the other, the time for the beam to reflect back is t. Therefore 2l = ct Beam of light mirror l t = 2l/c

Length Contraction 2 Observer on moving train with velocity, v : The time for the light to travel from the source to the mirror will be t 1 Distance from source to mirror = ct 1 = l’ + vt 1 Start point mirror l’ + vt 1 l’ ct 1 -vt 1 =l’ t 1 (c-v) =l’ t 1 = l’ / ( c-v)

Length Dilation 3 Consider now the beam of light after reflection : The measured time is t 2 Distance back from the mirror is ct 2 = l’ –vt 2 l’ - vt 1 l’ ct 2 +vt 2 = l’ t 2 (c+v) =l’ t 2 = l’/(c+v)

Length Contraction 4 For the moving observer the total time to measure the length is t 1 + t 2 =t’ t’= l’ / ( c-v) + l’/(c+v) A bit of heavy algebra

Length Contraction 5 The Algebra gets seriously scary here : We end up with l = length measured by stationary observer l’ = length measured by observer moving at constant velocity,v,relative to stationary observer

Length Contraction 6 Example Luke Skywalker, a stationary observer, measures a stationary racing pod to be 4m long. What length will ET travelling at a constant 0.5c, relative to Luke, measure the pod to be ? l = 4m v = 0.5c Equally Luke would observe ET to be shorter than Et measures himself to be.

Experimental Verification Cosmic rays collide with atoms in the earth’s upper atmosphere. This produces particles called MUONS, in the lab they have a mean lifetime of 2.2 μ s. The muons travel at 99.9%c. They would travel 650m. BUT substantial numbers are detected at sea level. In our reference frame the lifetime has been extended to 9 μs AND we measure the distance they travel as 60 km but in the reference frame of the muons the distance travelled is considerably smaller. When an atomic clock is flown around the world very fast, there is a measurable time dilation.

E = mc 2 Newton considered mass to be conserved BUT…… If a Luke Sywalker crashes the Millenium Falcon into the stationary Death Star, the damage caused will depend on the momentum of the Millenium Falcon. The change in momentum measured by Luke will be the same as that measured by Darth Vader on the Death Star. BUT they will both measure different velocities for the Millenium Falcon, the change in momentum is the same therefore Luke and Darth Vader must consider the mass of the Millenium Falcon to be different………………

E = mc 2 I showed that there is a mass /energy equivalence As the inertial mass increases with speed it requires more and more energy to increase the speed. No mass can travel at the speed of light as it would require an infinite amount of energy.