Pay close attention... because

Similar documents
Special Relativity 1

E = mc 2. Inertial Reference Frames. Inertial Reference Frames. The Special Theory of Relativity. Slide 1 / 63. Slide 2 / 63.

Special Theory of Relativity. The Newtonian Electron. Newton vs. Einstein. So if Newtonian Physics is wrong. It is all Relative.

RELATIVITY. Special Relativity

Two postulates Relativity of simultaneity Time dilation; length contraction Lorentz transformations Doppler effect Relativistic kinematics

Announcement. Einstein s Postulates of Relativity: PHYS-3301 Lecture 3. Chapter 2. Sep. 5, Special Relativity

Chapter 26 Special Theory of Relativity

RELATIVITY. Special Relativity

Name the object labelled B and explain its purpose.

Chapter 36 The Special Theory of Relativity. Copyright 2009 Pearson Education, Inc.

Chapter 1. Relativity 1

PHYSICS - CLUTCH CH 34: SPECIAL RELATIVITY.

Elements of Physics II

Lecture 8 : Special Theory of Relativity

Newtonian or Galilean Relativity

Relativity. April 16, 2014 Chapter 35 1

Relativity and Modern Physics. From Last Time. Preferred reference frame. Relativity and frames of reference. Galilean relativity. Relative velocities

Physics 2D Lecture Slides Lecture 2. Jan. 5, 2010

Introduction to Relativity & Time Dilation

Chapter 26. Relativity

Lecture 7: Special Relativity I

Notes - Special Relativity

Special Relativity 05/09/2008. Lecture 14 1

College Physics B - PHY2054C. Special Relativity 11/10/2014. My Office Hours: Tuesday 10:00 AM - Noon 206 Keen Building.

Relativity. An explanation of Brownian motion in terms of atoms. An explanation of the photoelectric effect ==> Quantum Theory

OPTION G SPECIAL AND GENERAL RELATIVITY. 0.5 c

2.3 The Lorentz Transformation Eq.

Our Dynamic Universe

Lorentz Transformation x = γ (x vt) y = y z = z t = γ (t vx/c 2 ) where γ 1/(1 - v 2 /c 2 ) 1/2

Unit 10: Relativity Hewitt Chapters Brent Royuk Phys-109 Concordia University

Chapter 37. Relativity. PowerPoint Lectures for University Physics, 14th Edition Hugh D. Young and Roger A. Freedman Lectures by Jason Harlow

Announcements. Muon Lifetime. Lecture 4 Chapter. 2 Special Relativity. SUMMARY Einstein s Postulates of Relativity: EXPERIMENT

Topics: Relativity: What s It All About? Galilean Relativity Einstein s s Principle of Relativity Events and Measurements

Before we work on deriving the Lorentz transformations, let's first look at the classical Galilean transformation.

CHAPTER 2 Special Theory of Relativity-part 1

Modern Physics. Third Edition RAYMOND A. SERWAY CLEMENT J. MOSES CURT A. MOYER

Physics 2D Lecture Slides Sept 29. Vivek Sharma UCSD Physics

Chapter 28: Relativity

Relating measurements in one reference frame to those in a different reference frame moving relative to the first

Modern Physics. t the end of the nineteenth century, many scientists believed that they had

The Constancy of the Speed of Light

More Relativity: The Train and The Twins

Chapter 3 Special relativity 3.1 About motion

Principle of Relativity

4/13/2015. Outlines CHAPTER 12 ELECTRODYNAMICS & RELATIVITY. 1. The special theory of relativity. 2. Relativistic Mechanics

Massachusetts Institute of Technology Physics Department Physics 8.20 IAP 2005 Introduction to Special Relativity

0 : Einstein s postulates of Special Relativity

Modern Physics. Relativity: Describes objects moving close to or at the speed of light (spaceships, photons, electrons )

Relativity. Overview & Postulates Events Relativity of Simultaneity. Relativity of Time. Relativity of Length Relativistic momentum and energy

Lesson 12 Relativity

2.4 The Lorentz Transformation

Correct Resolution of the Twin Paradox

Einstein s theory of special relativity

PHSC 1053: Astronomy Relativity

Physics 2D Lecture Slides Lecture 2. March 31, 2009

Physics. Special Relativity

Lecture Presentation Chapter 27 Relativity

Chapter 10: Special Relativity

Albert Einstein ( )

A100H Exploring the Universe: Black holes. Martin D. Weinberg UMass Astronomy

The result is; distances are contracted in the direction of motion.

Relativity. Physics April 2002 Lecture 8. Einstein at 112 Mercer St. 11 Apr 02 Physics 102 Lecture 8 1

Physics 2D Lecture Slides Lecture 4. April 3, 2009

12:40-2:40 3:00-4:00 PM

Lecture Notes (Einstein's Relativity)

Physics 107: Ideas of Modern Physics

Tuesday, February 15, Ice Cube Neutrino Facility

8.20 MIT Introduction to Special Relativity IAP 2005 Tentative Outline

Extra notes on rela,vity. Wade Naylor

Elements of Physics II

Theory of Relativity Final Quiz July 11, VERY short answers. Each worth 1 point.

College Physics B - PHY2054C. Special & General Relativity 11/12/2014. My Office Hours: Tuesday 10:00 AM - Noon 206 Keen Building.

The Foundations of Special Relativity

Module 2: Special Theory of Relativity - Basics

Relative Motion. Red Car sees Blue Car travel at U Blue Car throws Ball at V' What is V the speed of the Ball seen by Red Car?

A100 Exploring the Universe: Black holes. Martin D. Weinberg UMass Astronomy

Physics 2203, Fall 2012 Modern Physics

Special Theory of Relativity. PH101 Lec-2

Physics 107: Ideas of Modern Physics

PHY152H1S Practical 10: Special Relativity

) 2 = Square of rest energy. E = "m o. c 2, or E = mc 2. Homework & Exam

Kinematics III. I. Comparing Measurements By Different Observers

Special Relativity: Basics

Special. Relativity. Todd Huffman. Steve

SMMG: Relativity. Jack S. Calcut III

New problem of twin paradox

CHAPTER 2 Special Theory of Relativity Part 2

PHYS 270-SPRING 2011 Dennis Papadopoulos LECTURE # 20 RELATIVITY I NEWTONIAN RELATIVITY GALILEAN TRANSFORMATIONS SIMULTANEITY APRIL 21, 2011

Therefore F = ma = ma = F So both observers will not only agree on Newton s Laws, but will agree on the value of F.

Chapter 37. PowerPoint Lectures for University Physics, Twelfth Edition Hugh D. Young and Roger A. Freedman. Lectures by James Pazun

Physics 107: Ideas of Modern Physics

On the Arbitrary Choice Regarding Which Inertial Reference Frame is "Stationary" and Which is "Moving" in the Special Theory of Relativity

Kinematics of special relativity

ENTER RELATIVITY THE HELIOCENTRISM VS GEOCENTRISM DEBATE ARISES FROM MATTER OF CHOOSING THE BEST REFERENCE POINT. GALILEAN TRANSFORMATION 8/19/2016

Relativity, Put To The Test

CHAPTER 2 Special Theory of Relativity

Physics 2D Lecture Slides Oct 1. Vivek Sharma UCSD Physics

Introduction. Classical vs Modern Physics. Classical Physics: High speeds Small (or very large) distances

2.1 Einstein s postulates of Special Relativity. (i) There is no ether (there is no absolute system of reference).

RELATIVITY. The End of Physics? A. Special Relativity. 3. Einstein. 2. Michelson-Morley Experiment 5

Transcription:

Pay close attention... because

Galilean Relativity

Galilean Relativity

I drive past a baseball field traveling north at 25 MPH. A player throws the ball south at a speed (relative to the ground) of 70 MPH. What is the speed of the ball in my inertial reference frame (assuming classical Galilean Relativity)? A: 25 MPH B: 45 MPH C: 70 MPH D: 74 MPH E: 95 MPH

Galilean Relativity Laws of physics should be the same in any inertial reference frame

Galilean Relativity z S y x

Conventions The velocity v is the velocity of the S frame origin as viewed by someone in S frame. Use u to represent the velocity of an object. We define our coordinates such that the x, y, and z directions are the same for both coordinate systems, v is always in the x direction, and the origins of the two coordinate systems overlap at time t = 0.

Galilean Transformations

Problems with Galilean Relativity Maxwell s equations describe light... But Different from other waves Speed the same in any reference frame Ether wind

Michelson & Morley: 1881, 1887

Michelson & Morley: 1881, 1887

Michelson & Morley: 1881, 1887

Michelson & Morley: 1881, 1887

Michelson & Morley: 1881, 1887

Michelson & Morley: 1881, 1887

Michelson & Morley: 1881, 1887

Michelson & Morley: 1881, 1887

Postulates Einstein s Relativity 1. The mathematical form of the laws of physics must be the same in every inertial reference frame. 2. The speed of light in vacuum is a constant, and is the same constant in every inertial reference frame.

Simple postulates, but with bizarre consequences

A Single Observer

A Single Observer

An Array of Observers

In Earth Reference Frame

In Earth Reference Frame

In Earth Reference Frame Both lightning bolts strike at the same time The observers on the ground conclude that the observer on the train sees the light from the right bolt before they see light from the left bolt.

In Train Reference Frame Either the observer on the train sees light from both beams at the same time or the lightning bolts didn t strike at the same time!

Simultaneity Things which happen simultaneously in one inertial reference frame do not have to occur simultaneously in a different inertial reference frame.

2 NEPHI 26:23 For behold, my beloved brethren, I say unto you that the Lord God worketh not in darkness.

Time Dilation

Time Dilation

Time Dilation

Time Dilation The inertial frame in which two events occur at the same place is known as the proper frame for the two events. Not all pairs of events have a proper frame! If two events occur in the same place, separated by a time Δt p light can travel a distance L = c Δt p / 2 and back. But in the frame of someone moving at a speed v relative to the proper frame, the light must travel further than L. So the time between the two events in the moving frame is larger than the time in the proper frame!

Thought Question Two people in different inertial frames measure the time between two events. In which frame will the time interval between two events be the shortest? A : The one moving fastest with respect to the lab B : The one moving slowest with respect to the lab C : The one in which the events occur furthest apart D : The one in which the events occur closest together E : It depends on other information.

Time Dilation t = γ t p γ = 1 1 v2 c 2

This has been verified... many times A muon created on earth at rest lives an average of 2.2 x 10-6 s (2.2 μs) A muon traveling at.990c lives an average of 1.56 x 10-5 s (15.6 μs)

Discussion question: The value of γ is 1 v 2 A. Less than 1 1 c 2 B. Greater than 1 C. Can be either depending on the velocity

The Twin Paradox

After the trip, which twin will be the oldest? A : The little twin who went into space B : The little twin who stayed home C : The little twin who had roast beef D : The little twin who had none E : They will be the same age

Length Contraction: Goslo s Frame

Length Contraction: Speedo s Frame

Who measures the proper time for the oneway trip to Planet X? A : Goslo B : Speedo C : Neither of them D : Both of them E : Miss Manners

Length Contraction

Length Contraction L = L p γ Proper frame is the one in which the object isn t moving

The Barn Door Paradox

Discussion question: A rocket, when measured at rest, is 47 meters long. How long will you measure it to be if flies past you at 0.70 c? A. 65.8 meters B. 33.6 meters C. 47 meters D. 1.4 meters E. None of the above

Discussion question: The crew of a spaceship watches a movie that is two hours long in a spacecraft that is moving at high speed through space. An Earthbound observer, who is watching the movie through a powerful telescope, measures the duration of the movie to be... Notice I wrote A. Less than 2 hours measure the duration rather than B. 2 hours see the movie. C. More than 2 hours Make sure you understand why!

According to the special theory of relativity, if a 30- year old astronaut is sent on a space mission is accelerated to speeds close to that of light, and then returns to earth after 20 years as measured on earth, what would be his biological age upon returning? A. Less than 50 years B. 50 years C. More than 50 years