eppt m2 introduction to relativity k young, physics department, cuhk the chinese university of hong...

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EPPT M2 INTRODUCTION TO RELATIVITY K Young, Physics Department, CUHK The Chinese University of Hong Kong

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Page 1: EPPT M2 INTRODUCTION TO RELATIVITY K Young, Physics Department, CUHK  The Chinese University of Hong Kong

EPPT M2

INTRODUCTION TO RELATIVITY

EPPT M2

INTRODUCTION TO RELATIVITY

K Young, Physics Department, CUHKThe Chinese University of Hong Kong

Page 2: EPPT M2 INTRODUCTION TO RELATIVITY K Young, Physics Department, CUHK  The Chinese University of Hong Kong

Chapter 1

INTRODUCTIONChapter 1

INTRODUCTION

Page 3: EPPT M2 INTRODUCTION TO RELATIVITY K Young, Physics Department, CUHK  The Chinese University of Hong Kong

Questions of interest in relativityQuestions of interest in relativity

Behavior of particles at high speeds 2

0E mc Energy / momentum of particles at high

speeds; their interactions Twin paradox; length contraction Black holes Cosmology; expansions of universe

Page 4: EPPT M2 INTRODUCTION TO RELATIVITY K Young, Physics Department, CUHK  The Chinese University of Hong Kong

Common ThemeCommon Theme

How does the same phenomenon appear to different observers?

How is the same phenomenon described in different coordinate systems?

Page 5: EPPT M2 INTRODUCTION TO RELATIVITY K Young, Physics Department, CUHK  The Chinese University of Hong Kong

ExampleExample

v

Page 6: EPPT M2 INTRODUCTION TO RELATIVITY K Young, Physics Department, CUHK  The Chinese University of Hong Kong

ObjectivesObjectives

Physics independent of coordinates Rotation of coordinates Principle of relativity Experimental basis Applications

Page 7: EPPT M2 INTRODUCTION TO RELATIVITY K Young, Physics Department, CUHK  The Chinese University of Hong Kong

Physics Independentof Coordinates

Physics Independentof Coordinates

Page 8: EPPT M2 INTRODUCTION TO RELATIVITY K Young, Physics Department, CUHK  The Chinese University of Hong Kong

Physics independentof coordinates

Physics independentof coordinates

Physics is absolute Coordinates are

arbitrary

Physics independent of coordinates

Page 9: EPPT M2 INTRODUCTION TO RELATIVITY K Young, Physics Department, CUHK  The Chinese University of Hong Kong

Coordinate TransformationsCoordinate Transformations

Page 10: EPPT M2 INTRODUCTION TO RELATIVITY K Young, Physics Department, CUHK  The Chinese University of Hong Kong

Rotation leads to vectorsRotation leads to vectors

x

y

x'y'

Page 11: EPPT M2 INTRODUCTION TO RELATIVITY K Young, Physics Department, CUHK  The Chinese University of Hong Kong

Moving coordinates leads to Special Relativity

Moving coordinates leads to Special Relativity

V

Page 12: EPPT M2 INTRODUCTION TO RELATIVITY K Young, Physics Department, CUHK  The Chinese University of Hong Kong

General transformation leads to General Relativity

General transformation leads to General Relativity

Page 13: EPPT M2 INTRODUCTION TO RELATIVITY K Young, Physics Department, CUHK  The Chinese University of Hong Kong

Rotation of coordinatesRotation of coordinates

Linear relationship Vectors and matrices Rotation matrix

Page 14: EPPT M2 INTRODUCTION TO RELATIVITY K Young, Physics Department, CUHK  The Chinese University of Hong Kong

3D notation3D notation

x

y

z

r x

y

z

p

p

p

p

r, p bold

, , x y zr Cartesian

Page 15: EPPT M2 INTRODUCTION TO RELATIVITY K Young, Physics Department, CUHK  The Chinese University of Hong Kong

Coordinates are relativeCoordinates are relative

cos

sin 0

x L x L

y L y

Study coordinate transformations

x'

y'

L

x

y

L

End point = r

linearly relatedx x

y y

Page 16: EPPT M2 INTRODUCTION TO RELATIVITY K Young, Physics Department, CUHK  The Chinese University of Hong Kong

cos

sin

x r

y r

r

y

x

y'

r

'x'

cos

cos( )

x r

r

sin

sin( )

y r

r

Page 17: EPPT M2 INTRODUCTION TO RELATIVITY K Young, Physics Department, CUHK  The Chinese University of Hong Kong

cos sin

sin cos

( )

x x

y

R

y

r

r

cos sinx y

cosc sios s n nir r

cos( )x r

sin( )y r

coss siin c s nor r

( sin ) cosx y

Page 18: EPPT M2 INTRODUCTION TO RELATIVITY K Young, Physics Department, CUHK  The Chinese University of Hong Kong

Properties of rotation matricesProperties of rotation matrices

cos sin( )

sin cosR

( ) ( ) ( )R R R

Addition theorem for sin, cos

( ) ( )TR R

Page 19: EPPT M2 INTRODUCTION TO RELATIVITY K Young, Physics Department, CUHK  The Chinese University of Hong Kong

cos sin cos sin

sin cos sin cos

cos sin

sin cos

Addition theoremAddition theorem

Page 20: EPPT M2 INTRODUCTION TO RELATIVITY K Young, Physics Department, CUHK  The Chinese University of Hong Kong

Principle of RelativityPrinciple of Relativity

Page 21: EPPT M2 INTRODUCTION TO RELATIVITY K Young, Physics Department, CUHK  The Chinese University of Hong Kong

Physical law: different observersPhysical law: different observers

Variables covariant Equation invariant Depends on linear transformation

Page 22: EPPT M2 INTRODUCTION TO RELATIVITY K Young, Physics Department, CUHK  The Chinese University of Hong Kong

Physical law: different observersPhysical law: different observers

( ) ( ) m R RF aa

F

mF a

m F a

x xF ma y yF ma

x xF ma y yF ma

Page 23: EPPT M2 INTRODUCTION TO RELATIVITY K Young, Physics Department, CUHK  The Chinese University of Hong Kong

Principle of relativityPrinciple of relativity

All valid laws of physics should take the same form in different coordinates systems invariance

All terms in valid equation must transform in the same way covariance

How do they transform?

Page 24: EPPT M2 INTRODUCTION TO RELATIVITY K Young, Physics Department, CUHK  The Chinese University of Hong Kong

Experimental basisExperimental basis

SR: Michelson-Morley experiment: The speed of light is the same for all

observersGR: All objects fall at the same acceleration in

a gravitational fieldBoth known to great precisionThought to be exact

Page 25: EPPT M2 INTRODUCTION TO RELATIVITY K Young, Physics Department, CUHK  The Chinese University of Hong Kong

Order of magnitude of effectOrder of magnitude of effect

Particle moving at speed v Speed of light c Dimensionless ratio

vc

8 13.0 10 msc

Page 26: EPPT M2 INTRODUCTION TO RELATIVITY K Young, Physics Department, CUHK  The Chinese University of Hong Kong

Order of magnitude of effectOrder of magnitude of effect

Sign of does not matter

Page 27: EPPT M2 INTRODUCTION TO RELATIVITY K Young, Physics Department, CUHK  The Chinese University of Hong Kong

Another expressionAnother expression2 2

21 2 2

v mv

c mc

KE2

rest energy

Page 28: EPPT M2 INTRODUCTION TO RELATIVITY K Young, Physics Department, CUHK  The Chinese University of Hong Kong

Order of magnitude of effectOrder of magnitude of effect

Gravity important in GR

2

PE

rest energy

Page 29: EPPT M2 INTRODUCTION TO RELATIVITY K Young, Physics Department, CUHK  The Chinese University of Hong Kong

ExampleExample

What is clock error (seconds/day) due to

speed

height

3 km

1000 km/hr

Page 30: EPPT M2 INTRODUCTION TO RELATIVITY K Young, Physics Department, CUHK  The Chinese University of Hong Kong

ApplicationsApplications

Page 31: EPPT M2 INTRODUCTION TO RELATIVITY K Young, Physics Department, CUHK  The Chinese University of Hong Kong

ApplicationsApplications

Relativistic kinematics and dynamics — collisions

Mass-energy equivalence Relation between E & M Theory of gravity

Page 32: EPPT M2 INTRODUCTION TO RELATIVITY K Young, Physics Department, CUHK  The Chinese University of Hong Kong

ApplicationsApplications

Astrophysics Cosmology Global Positioning System (GPS) Constraining other laws of physics

Page 33: EPPT M2 INTRODUCTION TO RELATIVITY K Young, Physics Department, CUHK  The Chinese University of Hong Kong

Relativistic kinematics & dynamicsRelativistic kinematics & dynamics

SS

SS

laws Newtonian Apply

Only need to do this once and for all

S

cv 9.0

S'

1sm3 v

Page 34: EPPT M2 INTRODUCTION TO RELATIVITY K Young, Physics Department, CUHK  The Chinese University of Hong Kong

Mass-energy equivalenceMass-energy equivalence

From relativistic kinematics & dynamics, new concept of E, P, m

Important for nuclear physics & high energy physics

20E mc

Page 35: EPPT M2 INTRODUCTION TO RELATIVITY K Young, Physics Department, CUHK  The Chinese University of Hong Kong

High energy physicsHigh energy physics

What is matter made of ? How do the constituents interact ?

To study experimentally Accelerate to high energy/speed Let them collide To probe short distance

Page 36: EPPT M2 INTRODUCTION TO RELATIVITY K Young, Physics Department, CUHK  The Chinese University of Hong Kong

Quantum Field TheoryQuantum Field Theory

When E > E0 =mc2, particles can be created / destroyed

Theoretical description requires relativistic quantum field theory

Page 37: EPPT M2 INTRODUCTION TO RELATIVITY K Young, Physics Department, CUHK  The Chinese University of Hong Kong

SB

Electricity MagnetismElectricity Magnetism

qv

S'

q

Page 38: EPPT M2 INTRODUCTION TO RELATIVITY K Young, Physics Department, CUHK  The Chinese University of Hong Kong

E

B

Charge

Moving charge

Page 39: EPPT M2 INTRODUCTION TO RELATIVITY K Young, Physics Department, CUHK  The Chinese University of Hong Kong

GravityGravity

If ao = g, cannot tell apart

If we understand transformation to an accelerating frame, then we understand gravity??

S S'ao

g

Page 40: EPPT M2 INTRODUCTION TO RELATIVITY K Young, Physics Department, CUHK  The Chinese University of Hong Kong

BUT

Page 41: EPPT M2 INTRODUCTION TO RELATIVITY K Young, Physics Department, CUHK  The Chinese University of Hong Kong

Astrophysics — gravity importantAstrophysics — gravity important

2 2 2~

U GM

Mc Rc

R

GMU

2

~

2~

Rc

GM

Page 42: EPPT M2 INTRODUCTION TO RELATIVITY K Young, Physics Department, CUHK  The Chinese University of Hong Kong

Black hole — heuristic derivationBlack hole — heuristic derivation

KE PE

R

GMmmv 2

2

1

M

m

R

Escape?

Page 43: EPPT M2 INTRODUCTION TO RELATIVITY K Young, Physics Department, CUHK  The Chinese University of Hong Kong

Black hole — heuristic derivationBlack hole — heuristic derivation

21

2

GMmmv

R Escape?

M

m

RMax speed = c

2

PE1 /

2 rest energy

GMm R

mc

21

2

GMmmc

R

Page 44: EPPT M2 INTRODUCTION TO RELATIVITY K Young, Physics Department, CUHK  The Chinese University of Hong Kong

Black hole — heuristic derivationBlack hole — heuristic derivation

2

PE 1

rest energy 2 Escape

M

m

R

2

PE 1

rest energy 2 Cannot

Escape

Page 45: EPPT M2 INTRODUCTION TO RELATIVITY K Young, Physics Department, CUHK  The Chinese University of Hong Kong

Black hole — heuristic derivationBlack hole — heuristic derivation

2

PE 1

rest energy 2

M

m

R

2

/ 1

2

GMm R

mc

02

2GMR R

c

Page 46: EPPT M2 INTRODUCTION TO RELATIVITY K Young, Physics Department, CUHK  The Chinese University of Hong Kong

Black hole — heuristic derivationBlack hole — heuristic derivation

Mixture of Newtonian + relativisticNot really legitimateOK for order-of -magnitude estimate

2

0

2GMR

cR

Page 47: EPPT M2 INTRODUCTION TO RELATIVITY K Young, Physics Department, CUHK  The Chinese University of Hong Kong

Global Positioning System (GPS)

Global Positioning System (GPS)

1

1012

11

19

3

2

155

4

6

20

14

13

7

8

9

21 16

18

17

observer

r

satellitev

Page 48: EPPT M2 INTRODUCTION TO RELATIVITY K Young, Physics Department, CUHK  The Chinese University of Hong Kong

GPSGPS

Accuracy ~ 10 m

Page 49: EPPT M2 INTRODUCTION TO RELATIVITY K Young, Physics Department, CUHK  The Chinese University of Hong Kong

GPSGPS

2 2 2~ ~

GM gR

Rc c

9287 10~1031010~

421 ~ 10 s

~30 km

day

Page 50: EPPT M2 INTRODUCTION TO RELATIVITY K Young, Physics Department, CUHK  The Chinese University of Hong Kong

CosmologyCosmology

Depends on gravity In detail: Einstein's theory

Page 51: EPPT M2 INTRODUCTION TO RELATIVITY K Young, Physics Department, CUHK  The Chinese University of Hong Kong

Constraining other laws of physicsConstraining other laws of physics

Laws must be invariant Limited possibilities

Page 52: EPPT M2 INTRODUCTION TO RELATIVITY K Young, Physics Department, CUHK  The Chinese University of Hong Kong

ObjectivesObjectives

Physics independent of coordinates Rotation of coordinates Principle of relativity Experimental basis Applications

Page 53: EPPT M2 INTRODUCTION TO RELATIVITY K Young, Physics Department, CUHK  The Chinese University of Hong Kong

AcknowledgmentAcknowledgment

I thank Miss HY Shik and Mr HT Fung for design