1 Relativity part 1. 2 Where Do We Come From? What Are We? Paul Gauguin (1897) Where Are We Going? Museum of Fine Arts, Boston.

Slides:



Advertisements
Similar presentations
Einsteins Special Theory of Relativity. Relative Motion ALL motion is relative Speeds are only measured in relation to other objects No way to determine.
Advertisements

Classical Relativity Galilean Transformations
Maxwell’s Equations: The Final Classical Theory Catherine Firth & Alexa Rakoski.
Theory of Special Relativity
Relativity Theories. The Principle of Relativity Although motion often appears relative, it’s logical to identify a “background” reference frame from.
Wednesday, Feb. 4, 2015PHYS , Spring 2014 Dr. Jaehoon Yu 1 PHYS 3313 – Section 001 Lecture #5 Wednesday, Feb. 4, 2015 Dr. Jaehoon Yu Einstein’s.
Chapter 14: Maxwell’s Theory By Katie Zerr and Kristin Walker Topics that will be covered: Electromagnetic Theory Displacement Current Michelson-Morley.
1 Special Relativity 2. 2 Topics l Recap l Length Contraction l Cosmic Ray Muons l Spacetime l Summary.
Harrison B. Prosper Florida State University Young Scholars Program.
Physics 3 for Electrical Engineering Ben Gurion University of the Negev
 PROGRAM OF “PHYSICS2B” Lecturer: Dr. DO Xuan Hoi Room A1. 413
Relativity Pierre-Hugues Beauchemin PHY 006 –Talloire, May 2013.
How I Learned To Stop Worrying About Speed and Love Light, or Prepared and Presented by Mauricio Campuzano GK-12 Fellow Stevens Institute of Technology.
INFINITE SPACE AND ABSOLUTE TIME. Large scale bubble-like structures in the universe. The image contains about 4000 galaxies each representing one luminous.
Chapter 22: Black Holes Einstein’s relativity: –Special –General –Relativity and black holes Evidence of black holes Properties of black holes Long-time.
26-1 Physics I Class 26 The Special Theory of Relativity* *This material is optional. It will not be on any exam.
Lecture 11 Special Theory of Relativity I ASTR 340 Fall 2006 Dennis Papadopoulos.
Lecture 12 Special Theory of Relativity II ASTR 340 Fall 2006 Dennis Papadopoulos.
Principle of special relativity Their is inconsistency between EM and Newtonian mechanics, as discussed earlier Einstein proposed SR to restore the inconsistency.
Special Theory of Relativity
1879 Born in Ulm, Germany Einstein receives his first compass, beginning his quest to investigate the natural world Albert attempts to skip high.
Special Relativity. Topics Motion is Relative Michelson-Morley Experiment Postulates of the Special Theory of Relativity Simultaneity Spacetime Time Dilation.
ALBERT EINSTEIN BORN MARCH 14, 1879 IN ULM, GERMANY. HE HAD 3 KIDS. HANS, EDUARD, AND LIESERL ALBERT.
Maxwell’s Theory Tom Catalano & Sam Roskos. James Clerk Maxwell ( ) Scottish mathematical physicist Vastly influential in many different fields.
Julia Sickels - jns5224 Sam Fisher - sef5176 Alyssa Hawras - aoh5295.
Amanda Dorsey Faranak Islam Jose Guevara Patrick Conlin
BY CARLO BECERRA & LUIS ALCAZAR Albert Einstein. Background o Born: Ulm, Kingdom of Wurttemberg, German Empire o March 14, 1879 o In 1901 he worked as.
Why does the mud fly off the tires of a pickup traveling down the interstate? Copernicus had difficulty convincing his peers of the validity of his heliocentric.
Announcements Homework: Supplemental Problems 2 nd Project is due at the final exam which is Tuesday May 5 at 1:30 – 3:30pm. A list of potential projects.
18 September 2001Astronomy 102, Fall Einstein at Caltech, 1933 Today in Astronomy 102: relativity In the next five lectures we will discuss Einstein’s.
M H Maps of space Space: N & E or M & H Electromagnetism: E & B or E & B.
RELATIVITY. Principle of Relativity Postulates of Relativity Special Theory of Relativity General Theory of Relativity.
Special and General Relativity Marcus Han 3O3 (!0)
2.1The Apparent Need for Ether 2.2The Michelson-Morley Experiment 2.3Einstein’s Postulates 2.4The Lorentz Transformation 2.5Time Dilation and Length Contraction.
Introduction to special relativity
Page 1 Phys Baski Relativity I Topic #9: Special Relativity I Transformation of Variables between Reference Frames –Non-relativistic Galilean Transformation.
Special relativity.
Einstein’s Special Theory of Relativity Dr. Zdzislaw Musielak UTA Department of Physics.
Little drops of water, little grains of sand, make the mighty ocean and the pleasant land. Little minutes, small though they may be, make the mighty ages.
25 September 2001Astronomy 102, Fall The world’s most famous patent clerk, c Today in Astronomy 102: relativity, continued  Einstein’s procedures.
Special Relativity The Failure of Galilean Transformations
Chapter 9 Relativity Basic Problems The formulation of Newtonian mechanics is based on our daily experience and observation. But, Newtonian mechanics.
It’s all Relativity. March, 1905: Twenty six year old Albert Einstein demonstrates the particle nature of light by explaining the photoelectric effect.
PHYS 221 Recitation Kevin Ralphs Week 12. Overview HW Questions Chapter 27: Relativity – History of Special Relativity (SR) – Postulates of SR – Time.
Announcements Exam 3 is scheduled for Wednesday April 8. Will be pushed back to Monday April 13 Tentatively will cover the rest of Chapter 4, all of Chapters.
Relativity: History 1879: Born in Ulm, Germany. 1901: Worked at Swiss patent office. –Unable to obtain an academic position. 1905: Published 4 famous.
Special Relativity I wonder, what would happen if I was travelling at the speed of light and looked in a mirror?
Relativity Jennifer Keehn. “I want to know how God created this world. I am not interested in this or that phenomena, in the spectrum of this or that.
Astronomy 1143 – Spring 2014 Lecture 18: Special Relativity.
Physics 12 MODERN PHYSICS: AN INTRODUCTION.  QUOTE AND CLIP OF.
The Michelson-Morley Experiment
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.
IB Physics – Relativity Relativity Lesson 1 1.Galilean Transformations (one frame moving relative to another) Michelson Morley experiment– ether. 2.Speed.
Special Relativity Physics 12 Adv. Einstein’s Postulates  In 1905, while working as a patent clerk in Switzerland, Einstein published his paper on.
Chapter 39 Relativity. A Brief Overview of Modern Physics 20 th Century revolution 1900 Max Planck Basic ideas leading to Quantum theory 1905 Einstein.
Wed., Sept. 5, 2012PHYS , Fall 2012 Dr. Jaehoon Yu 1 PHYS 3313 – Section 001 Lecture #3 Wednesday, Sept. 5, 2012 Dr. Jaehoon Yu Galilean Transformation.
Special Theory of Relativity. Galilean-Newtonian Relativity.
Special Relativity By Jackson Andrews.
1 PHYS 3313 – Section 001 Lecture #4 Monday, Jan. 27, 2014 Dr. Jaehoon Yu Galilean Transformation Do we need Ether? Michelson-Morley Experiment Einstein’s.
Relativity. Historical Development 1600s Newton discovered his laws of mechanics Applied to a wide variety of problems over the next two decades Worked.
Special Relativity How does light behave in moving reference 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.
PHYS 342: More info The TA is Meng-Lin Wu: His is His office hour is 10:30am to 12pm on Mondays His office is Physics.
UNIT-III RIGID BODY DYNAMICS
Albert Einstein and the Theory of Relativity
Einstein’s Relativity Part 2
Einstein’s Life! Created by Educational Technology Network
The Special Theory of Relativity*
Special Theory Of Relativity Represented By
Presentation transcript:

1 Relativity part 1

2 Where Do We Come From? What Are We? Paul Gauguin (1897) Where Are We Going? Museum of Fine Arts, Boston

3 Topics l A Glorious “Failure” l Special Relativity l Summary

4 A Glorious “Failure”

5 James Clerk Maxwell ( ) Maxwell’s Equations describing electric and magnetic fields in a vacuum.

6 Electro + Magnetism = Light medium ”We can scarcely avoid the conclusion that light consists in the transverse undulations of the same medium which is the cause of electric and magnetic phenomena.” Maxwell (1866) Moreover, light travels at a specific speed in aether300,000 km/s this medium (the aether): 300,000 km/s

7 The Aether Wind Taking the stars as our reference, the Earth 30 km/s travels at about 30 km/s around the Sun. Therefore, it was argued (in the late 1870s), the aether should be flowing past us at a speed close 30 km/s to 30 km/s, since the aether is surely at rest relative to the stars.

8 Swimming The Aether Sea ac b w Michelson’s clever idea: Speed of water relative to bank: 3 ft/s Speed of swimmer relative to water: 5 ft/s Who wins the race?

9 Measuring The Aether Wind Michelson Experiment (1881) Michelson-Morley Experiment (1887)

10 A Glorious “Failure” “The interpretation of these results is that there is no displacement of the interference bands. … The result of the hypothesis of a stationary aether is thus shown to be incorrect.” A. A. Michelson, Am. J. Sci., 122, 120 (1881) Nobel Prize 1907!

11 The Lorentz-FitzGerald Theory FitzGerald ( ) Lorentz ( )

12 Special Relativity 1905

13 14 March, 1879, Ulm, Germany Hermann Einstein Pauline Einstein Albert

14 Aarau Class of 1896 From , Einstein was enrolled at the Eidgenössische Technische Hochschule, Zurich Marcel Grossman

15 Technical Expert, Third Class Einstein got a job at the Swiss Patent Office in Bern, on the 23 June 1902 Six months later, he married his Serbian girlfriend, Mileva

– Annus Mirabilis l 17 March l A new theory of light l 30 April l A new method to infer the size of molecules l 11 May l A new theory of Brownian motion l 30 June l A new theory of space and time

17 Special Relativity Principles l The Principle of Relativity: The laws of physics are the same in all inertial frames of reference l The speed of light, in vacuum, is independent of the motion of its source It follows from the above that the speed of light must be independent of the motion of the observer, also.

18 Time Dilation c T v T d (c  T) 2 = (v  T) 2 + d 2 T = time in frame in which clock is moving

19 Time Dilation – II Stationary clock frame d = c t Moving clock frame (c  T) 2 = (v  T) 2 + d 2 t =T /  t = time in frame in which clock is stationary

20 Length Contraction You:D = v T d = v t d / t = v = D / Td = D / (T / t) d = D /  Prof

21 Time Dilation and Length Contraction Moving clocks tick more slowly Moving lengths contract T is time in moving clock frame t is time in stationary clock frame D is length in stationary object frame d is length in moving object frame

22 Moving clocks run more slowly! Moving objects shorten! But, what Einstein recognized is that this effect must, by the principle of relativity, be perfectly symmetrical between different frames of reference.

23 Cosmic Ray Muons ~ 20 km Muon lifetime 2 ~ 2 microsecond Time to the ground 20km / 300,000 km/s 70 ~ 70 microsecond For every 35 microseconds of our clock, the muon’s “clock” advances only 1 microsecond!

24 Space + Time = Spacetime The distinction between past, present and future is only an illusion, even if a stubborn one. Albert Einstein

25 Earth’s Time Axis 3007 AD 2007 AD 2507 AD y x now Event: A place at a given time Spacetime: The set of all events (t,x,y,z) A B CD O

26 Summary l Michelson found no evidence of motion through an aether. l Lorentz and Fitzgerald proposed a clever, but ad hoc, theory to explain the result l Einstein’s theory is based on two principles: l Principle of relativity l Principle of relativity: The laws of physics are the same in all inertial frames of reference l The speed of light is independent of the motion of the light source