Physics 2D Lecture Slides Jan 10. Vivek Sharma UCSD Physics

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

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

Physics 2D Lecture Slides Lecture 3. January 8, 2010

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

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

Physics 2D Lecture Slides Lecture 5: Jan 12th 2004

1st Year Relativity - Notes on Lectures 3, 4 & 5

Prelims 1997 Question 6

CHAPTER 2 Special Theory of Relativity-part 1

Consequences of special relativity.

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

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

Special Theory of Relativity. PH101 Lec-3

Consequences of special relativity.

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

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

The Lorentz Transformations

2.4 The Lorentz Transformation

Analyzing the Twin-Paradox

Relativity Albert Einstein: Brownian motion. fi atoms. Photoelectric effect. fi Quantum Theory On the Electrodynamics of Moving Bodies

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

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

Paradoxes in Special Relativity Paradoxes in Special Relativity. Dr. Naylor

Lecture 10: General Relativity I

Extra notes on rela,vity. Wade Naylor

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

Lecture 10: General Relativity I

2.3 The Lorentz Transformation Eq.

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

Unit- 1 Theory of Relativity

Lecture 4 - Lorentz contraction and the Lorentz transformations

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

Wallace Hall Academy

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

DOPPLER EFFECT FOR LIGHT DETECTING MOTION IN THE UNIVERSE HUBBLE S LAW

Today. life the university & everything. Reminders: Review Wed & Fri Eyes to the web Final Exam Tues May 3 Check in on accomodations

Chapter 1. Relativity 1

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

Doppler shift and aberration for spherical electromagnetic waves

Gravitation and Cosmology

Recall from last time

General Physics I. Lecture 21: Relativistic Energy and Momentum. Prof. WAN, Xin ( 万歆 )

Newtonian or Galilean Relativity

The Cosmic Distance Ladder. Hubble s Law and the Expansion of the Universe!

Special Relativity 1

Relativity. April 16, 2014 Chapter 35 1

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

Modern Physics notes Spring 2005 Paul Fendley Lecture 37

SPH4U UNIVERSITY PHYSICS

Special Relativity 05/09/2008. Lecture 14 1

More Relativity: The Train and The Twins

Modern Physics Part 2: Special Relativity

Principle of Relativity

λ λ CHAPTER 7 RED-SHIFTS AND ENERGY BALANCE Red-shifts Energy density of radiation Energy density of matter Continuous creation 7.

Lecture Notes on Relativity. Last updated 10/1/02 Pages 1 65 Lectures 1 10

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

Summary: Mathematical Atomism (Unified Revolution: New Fundamental Physics) compared to Mainframe Physics. By Espen Gaarder Haug

the evidence that the size of the observable Universe is changing;

Kinematics of special relativity

Massachusetts Institute of Technology Physics Department

Physics H7C Midterm 2 Solutions

Advantages of Three-Dimensional Space-Time Frames

Line Spectra / Spectroscopy Applications to astronomy / astrophysics

The Theory of Relativity

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

Learning Objectives. distances to objects in our Galaxy and to other galaxies? apparent magnitude key to measuring distances?

Special Relativity: What Time is it?

Questions on Universe

The Cosmic Microwave Background

I bully myself cause I make me do what I put my mind to. -Marshall Mathers

Massachusetts Institute of Technology Department of Physics. Physics Out: Friday 29 September 2006 Due: Friday 6 October 2006.

Astronomy 114. Lecture35:TheBigBang. Martin D. Weinberg. UMass/Astronomy Department

2011 Arizona State University Page 1 of 6

The Contents of the Universe (or/ what do we mean by dark matter and dark energy?)

The Foundations of Special Relativity

Lecture Outline Chapter 29. Physics, 4 th Edition James S. Walker. Copyright 2010 Pearson Education, Inc.

Notes - Special Relativity

Observations versus Measurements

SPECIAL RELATIVITY. Introduction:

Einstein for Everyone Lecture 4: Paradoxes; Minkowski Spacetime

Lesson 12 Relativity

Exam. Topics covered in Exam 2. Wave properties. Types of wave motion. Waves Questions. Interference of sound waves

Gravitational Effects on Light Propagation. Copyright 2009 Joseph A. Rybczyk

Chapter 26 Special Theory of Relativity

The Doppler Effect is the change in frequency observed when a source of sound waves is moving relative to an observer.

Physics 2D Lecture Slides Lecture : Jan 11th 200. First Quiz This Friday!

Today: Start Ch. 18: Cosmology. Homework # 5 due next Wed. (HW #6 is online)

Lecture 13 Notes: 07 / 20. Invariance of the speed of light

Talking about general relativity Important concepts of Einstein s general theory of relativity. Øyvind Grøn Berlin July 21, 2016

Welcome back to Physics 215

( ) 2 + v t B = 2 D2 + L 2. = 2D c. t B. & t A. , L = v t B. D = c t A. + v t. = t A. = 2 c. c 2. ( v2 c ) = t. 1 v2. t B 2 = t A.

Dark Energy in Our Expanding Universe Joe Mohr Department of Astronomy Department of Physics NCSA

Lecture 2 - Length Contraction

Today s class. The optical Doppler effect Excursion to the universe!

Unit 1. The Expanding Universe

Physics 8.20 Special Relativity IAP 2008

Spectroscopy in Motion: A Method to Measure Velocity

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

Modern Physics notes Paul Fendley Lecture 34. Born, chapter III (most of which should be review for you), chapter VII

Transcription:

Physics D Lecture Slides Jan 10 Vivek Sharma UCSD Physics

Time Dilation Example: Relativistic Doppler Shift Light : velocity c = f λ, f=1/t A source of light S at rest Observer S approches S with velocity v S measures f or λ, c = f λ Expect f > f since more wave crests are being crossed by Observer S due to its approach direction than if it were at rest w.r.t source S

Relativistic Doppler Shift λ'=ct'-vt', use f = c/ λ c T f ' =, T ' = (c-v)t' 1- (v/c) Substituting for T', use f=1/t Examine two successive wavefronts emitted by S at location 1 and In S frame, T = time between two wavefronts In time T, the Source moves by ct w.r.t 1 Meanwhile Light Source moves a distance vt Distance between successive wavefront λ = ct vt f ' = 1- (v/c) 1- (v/ c) 1+(v/c) f ' = f 1-(v/c) better remembered as: 1+(v/c) f obs = fsource 1-(v/c) f obs = Freq measured by observer approching light source

1+(v/c) f = f obs 1-(v/c) source

Doppler Shift & Electromagnetic Spectrum RED BLUE

Emission & Absorption Spectra of Atoms: DNA

Spectral Lines and Tracking Moving Objects

Doppler Shift in Spectral Lines and Motion of Radiating Objects Laboratory Spectrum, lines at rest wavelengths Lines Redshifted, Object moving away from me Larger Redshift, object moving away even faster Lines blueshifted, Object moving towards me Larger blueshift, object approaching me faster

The Cosmological Redshift The Expanding Universe: Space itself is Expanding

Cosmological Redshift As Universe expands EM waves stretch in Wavelength

Seeing Distant Galaxies Thru Hubble Telescope Through center of a massive galaxy clusters Abell 1689

Expanding Universe, Edwin Hubble & Mount Palomar Hale Telescope, Mount Palomar Edwin Hubble 190 Expanding Universe

Galaxies at different locations in our Universe travel at different velocities

Hubble s Measurement of Recessional Velocity of Galaxies V = H d : Farther things are faster they go H = 75 km/s/mpc (3.08x10 16 m) Play the movie backwards! Our Universe is about 10 Billion Years old

Now for Something Totally Different : Paradox! A paradox is an apparently self-contradictory statement, the underlying meaning of which is revealed only by careful scrutiny. The purpose of a paradox is to arrest attention and provoke fresh thought ``A paradox is not a conflict within reality. It is a conflict between reality and your feeling of what reality should be like.'' - Richard Feynman Construct a few paradoxes in Relativity & analyze them

Jack and Jill s Excellent Adventure: Twin Paradox Jill sees Jack s heart slow down Factor : 1 ( v/ c) = = 1 (0.8 c/ c) 0.6 For every 5 beats of her heart She sees Jack s beat only 3! Jack has only 3 thoughts for 5 that Jill has! Every things slows! Finally Jack returns after 50 yrs gone by according to Jill s calendar Only 30 years have gone by Jack Jack is 50 years old, Jane is 70! Jack & Jill are 0 yr old twins, with same heartbeat Jack takes off with V = 0.8c to a star 0 light years away Jill stays behind, watches Jack by telescope Is there a paradox here??

Twin Paradox? Paradox : Turn argument around, motion is relative Jack claims he at rest, Jill is moving v=0.8c Should not Jill be 50 years old when 70 year old Jack returns from space Odyssey? No! because Jack is not traveling in a inertial frame of reference TO GET BACK TO EARTH HE HAS TO TURN AROUND => decelerate/accelerate But Jill always remained in Inertial frame Time dilation formula applies to Jill s observation of Jack but not to Jack s observation of Jill Non-symmetric aging verified with atomic clocks taken on airplane trip around world and compared with identical clock left behind. Observer who departs from an inertial system will always find its clock slow compared with clocks that stayed in the system

Round The World With An Atomic Clock Atomic Clock : certain transitions in Cesium atom Two planes take off from DC, travel east and west Eastward trip took 41. hrs Westward trip took 48.6 Atomic clocks compared to similar ones kept in DC Need to account for Earth s rotation + GR etc Travel Predicted Measured Eastward Westward -40 ± 3 ns 75 ± 1 ns -59 ± 10 ns 73 ± 7 ns Flying clock ticked faster or slower than reference clock. Slow or fast is due to Earth s rotation

V = (3/5)c Fitting a 5m pole in a 4m barnhouse S t D Student u dfarmboy Farmboy says You e can do it n Student says Dude, t you are nuts d e c i Student with pole runs with v=(3/5) c farmboy sees pole contraction factor 1 (3c c = /5 ) 4/5 says pole just fits in the barn fully! Student with pole runs with v=(3/5) c Student sees barn contraction factor c c = 1 (3 /5 ) 4/5 says barn is only 3.m long, too short to contain entire 5m pole! Is there a contradiction? Is Relativity wrong? Homework: You figure out who is right, if any and why. Hint: Think in terms of observing two events Arrival of left end of pole at left end of barn Arrival of right end of pole at right end of barn

Discovering The Correct Transformation Rule Need to figure out x' = x vt guess x' = G( x vt) x = x' + vt' guess x = G( x' + vt' ) Do a Thought Experiment: Rocket Motion along x axis functional form of G! G must be dimensionless G does not depend on x,y,z,t But G depends on v/c G is symmetric As v/c 0, G 1 Rocket in S (x,y,z,t ) frame moving with velocity v w.r.t observer on frame S (x,y,z,t) Flashbulb mounted on rocket emits pulse of light at the instant origins of S,S coincide That instant corresponds to t = t = 0. Light travels as a spherical wave, origin is at O,O Speed of light is c for both observers Examine a point P (at distance r from O and r from O ) on the Spherical Wavefront The distance to point P from O : r = ct The distance to point P from O : r = ct Clearly t and t must be different t t

Discovering Lorentz Transfromation for (x,y,z,t) Motion is along x-x axis, so y, z unchanged y =y, z = z Examine points x or x where spherical wave crosses the horizontal axes: x = r, x =r x = ct = G( x' + vt') x' = ct' = G( x - vt), G t' = ( x- vt) c x = ct = G( ct ' + vt ') v = + c c = G [ c v ] 1 or G = = γ 1 ( v/ c) ct G ( ct vt) vt t x' = γ ( x vt) x' = γ ( x vt), x= γ ( x' + vt') x = γγ ( ( x vt) + vt ') γ + γ = γ x x vt vt ' x γ x γ vt x x t' = + γ t γv γv γv = + γ v v x 1 1 v t' = γ t+ 1, since 1 = v γ γ c x v t ' = γ vx t + [1 1 γ = t v c c

Lorentz Transformation Between Ref Frames ' ' ' ' ( ) y y z z v t t x t c x v x γ γ = = = = Lorentz Transformation ' ' ' ) ' ' ( y y z v t x x v t c t x z γ γ = + = = + = Inverse Lorentz Transformation As v 0, Galilean Transformation is recovered, as per requirement Notice : SPACE and TIME Coordinates mixed up!!!