1. Special Relativity The Failure of Galilean Transformations
The Lorentz Transformation
Time and Space in Special Relativity
Relativistic Momentum and Energy

2. The Galilean Transformations
Consider the primed coordinate system moving along the x-axis at speed u. Consider events where clocks record the time at the location of the event.
Galilean Transformation between coordinate systems
x’=x-ut
y’=y
z’=z
t’=t
vx’=vx-u
vy’=vy
vz’=vz

3. “The Ether” and the Michelson-Morley Experiment
What about light? Waves must be waving something…
The Ether…An absolute reference frame?
Should be able to detect and measure Earth’s motion through the ether by detecting an “ether wind” that should modify the speed of light along and transverse to the “wind” direction.

4. “The Ether” and the Michelson-Morley Experiment
Michelson-Morley detected no change in speed of light…
Galilean Transformations not correct for light !!!!

5. Einstein’s Postulates of Special Relativity
A reference frame in which a mass point thrown from the same point in three different (non co-planar) directions follows rectilinear paths each time it is thrown, is called an inertial frame.
– L. Lange (1885) as quoted by Max von Laue in his book (1921) Die Relativitätstheorie, p. 34, and translated by Iro).
The Principle of Relativity. The laws of physics are the same in all inertial reference frames.
The Constancy of the Speed of Light. Light moves through vacuum at a constant speed c that is independent of the motion of the light source.

6. The Lorentz Transformations

7. The Lorentz Transformations
Constancy of speed of light can be satisfied if space-time coordinates satisfy the linear Lorentz-Transformation equations…
Lengths perpendicular to are unchanged
Coefficients determined by invoking symmetry arguments and Einstein’s postulates ….

8. The Lorentz Transformations Time coordinate
Invoking the constancy of speed of light. Consider flash of light set off at t’=t=0 at common origins. At a later time t an observer in frame S will measure a spherical wavefront of light with radius ct, moving away from the origin and satisfying:
Similarly, at a time t’, an observer in frame S’ will measure a spherical wavefront of light with radius ct’, moving away from the origin O’ with speed c and satisfying :
Inserting equations into 4.15 and comparing with 4.14
t’ should be the same if y-->-y or z-->-z.
Consider motion of the origin O’ of frame S’. Synchronized at t=t’=0. x-coordinate of O’ is given by x=ut in frame S, and x’=0 in frame S’.
At this point:

9. The Lorentz Transformations
Reveal that
Lorentz Factor
Thus the Lorentz transformations linking the space and time coordinates (x,y,z,t) and (x’,y’,z’,t’) of the same event measured from S and S’ are
When ,relativistic formulas must agree with Newtonian equations….

10. The Lorentz Transformations
Array Representation:
Four-dimensional space-time
Space and time “mix” !!!!
for light wave x=ct,x’=ct’,x”=ct”,….
Minkowski Diagram

11. Electromagnetic Wave Equation
Galilean Transformation
Lorentz Transformation

12. Space-Time Interval Time-like interval Space-like interval
(interval)2=(separation in time)2-(separation in space)2
Space-time interval is invariant
Time-like interval
Space-like interval
Light-Like Interval
Causality

13. Space-Time Diagrams

15. Relativity of Simultaneity
Observer in S measures two flash-bulbs going off at same time t but at different locations x1and x2. Then an observer in S’ would measure the time interval between the two flashes as:
Events that occur in simultaneously in one inertial frame do NOT occur simultaneously in all other inertial reference frames

16. Proper Time And Time Dilation

17. Proper Length and Length Contraction
Measure positions at endpoints at same time in frame S’ and in frame S, L’=x2’-x1’

19. Example of Time Dilation and Length Contraction: Cosmic Ray Muons