EPPT M2 INTRODUCTION TO RELATIVITY K Young, Physics Department, CUHK The Chinese University of Hong Kong
Chapter 1 INTRODUCTION
Questions of interest in relativity Behavior of particles at high speeds Energy / momentum of particles at high speeds; their interactions Twin paradox; length contraction Black holes Cosmology; expansions of universe
Common Theme How does the same phenomenon appear to different observers? How is the same phenomenon described in different coordinate systems?
Example v
Objectives Physics independent of coordinates Rotation of coordinates Principle of relativity Experimental basis Applications
Physics Independent of Coordinates
Physics independent of coordinates Physics is absolute Coordinates are arbitrary Physics independent of coordinates
Coordinate Transformations
Rotation leads to vectors x y x' y'
Moving coordinates leads to Special Relativity V
General transformation leads to General Relativity
Rotation of coordinates Linear relationship Vectors and matrices Rotation matrix
3D notation bold Cartesian
Coordinates are relative Study coordinate transformations x' y' L x y L End point = r
r y x y' r '' x'
Properties of rotation matrices Addition theorem for sin, cos
Addition theorem
Principle of Relativity
Physical law: different observers Variables covariant Equation invariant Depends on linear transformation
Physical law: different observers a F
Principle 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?
Experimental basis SR: Michelson-Morley experiment: The speed of light is the same for all observers GR: All objects fall at the same acceleration in a gravitational field Both known to great precision Thought to be exact
Order of magnitude of effect Particle moving at speed v Speed of light c Dimensionless ratio v c
Order of magnitude of effect Sign of does not matter
Another expression
Order of magnitude of effect Gravity important in GR
Example What is clock error (seconds/day) due to speed height 3 km 1000 km/hr
Applications
Relativistic kinematics and dynamics — collisions Mass-energy equivalence Relation between E & M Theory of gravity
Applications Astrophysics Cosmology Global Positioning System (GPS) Constraining other laws of physics
Relativistic kinematics & dynamics Only need to do this once and for all SS'
Mass-energy equivalence From relativistic kinematics & dynamics, new concept of E, P, m Important for nuclear physics & high energy physics
High 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
Quantum Field Theory When E > E 0 =mc 2, particles can be created / destroyed Theoretical description requires relativistic quantum field theory
S B Electricity Magnetism q v S' q
Gravity =If a o = g, cannot tell apart =If we understand transformation to an accelerating frame, then we understand gravity?? SS' aoao g
BUT
Astrophysics — gravity important
Black hole — heuristic derivation M m R Escape?
Black hole — heuristic derivation Escape? M m R Max speed = c
Black hole — heuristic derivation Escape M m R Cannot Escape
Black hole — heuristic derivation M m R
Mixture of Newtonian + relativistic Not really legitimate OK for order-of -magnitude estimate
Global Positioning System (GPS)
GPS Accuracy ~ 10 m
GPS
Cosmology =Depends on gravity =In detail: Einstein's theory
Constraining other laws of physics =Laws must be invariant =Limited possibilities
Objectives =Physics independent of coordinates =Rotation of coordinates =Principle of relativity =Experimental basis =Applications
Acknowledgment =I thank Miss HY Shik and Mr HT Fung for design