By:%20Jennifer%20Doran - PowerPoint PPT Presentation

About This Presentation
Title:

By:%20Jennifer%20Doran

Description:

A star cruiser is moving away from the planet Mars with a speed of 0.58c and ... 0.69c = the velocity of the rocket in the reference frame of the star cruiser ... – PowerPoint PPT presentation

Number of Views:37
Avg rating:3.0/5.0
Slides: 36
Provided by: CPC
Learn more at: http://www.hep.fsu.edu
Category:

less

Transcript and Presenter's Notes

Title: By:%20Jennifer%20Doran


1
Relativity
  • By Jennifer Doran

2
What was Known in 1900
  • Newtons laws of motion
  • Maxwells laws of electromagnetism

3
Contradiction Between Laws
  • Newtons Laws
  • Predicted that the speed of light should depend
    on the motion of the observer and the light source
  • Maxwells Laws
  • Predicted that light in a vacuum should travel
    at a constant speed regardless of the motion of
    the observer or source

4
Two Postulates of Special Relativity
  • The laws of physics are the same for all
    non-accelerating observers
  • The speed of light in a vacuum is constant for
    all observers, regardless of motion

5
Inconsistencies with Classical Mechanics
  • Newtons Laws state that vuV
  • Einsteins postulate says that the speed of light
    is independent of the motion of all observers and
    sources.

6
Classical Lorentz Transformation
  • x x' u t' y y' z z' t t' OR
  • x' x u t y y' z z' t t'
  • Then v v' u
  • And a a'
  • BUT this is only good for ultltv.
  • To make the transforms relativistic, assume
  • x G (x' u t')
  • x' G (x u t)

7
Finding G
  • A light pulse starts at S at t 0 S' at t' 0
  • So in S, x ct, and in S, x c t', by
    Einsteins second postulate
  • Then ct G (c t' u t') G (c u) t'
  • And ct' G (c - u) t
  • Substitute for t', then ct G(c u)G(c -
    u)t/c
  • Then G2 c2 / (c2-u2) 1/(1- u2/c2)
  • G 1/v(1- u2/c2)

8
Time Dilation
  • ?t G?tp
  • ?tp is the proper time, the time between events
    which happen at the same place.
  • Since G is always greater than 1, all clocks run
    more slowly according to an observer in relative
    motion.

9
Time Dilation Example
  • An astronaut in a spaceship traveling away from
    the earth at u 0.6c decides to take a nap. He
    tells NASA that he will call them back in 1 hour.
    How long does his nap last as measured on earth?

10
Time Dilation Example
  • ?tp 1 hour
  • 1 (u/v)2 1 (0.6)2 0.64
  • Therefore, G v(1/0.64) 1.25
  • ?t 1.25 hours

11
Length Contraction
  • L (1/G)Lp
  • Lp is the length of the object in the reference
    frame in which the object is at rest.
  • All observers in motion relative to the object
    measure a shorter length, but only in the
    direction of motion.

12
Length Contraction
13
Length Contraction Example
  • In the reference frame of a muon traveling at u
    0.999978c, what is the apparent thickness of
    the atmosphere? (To an observer on earth, the
    height of the atmosphere is 100 km.)

14
Length Contraction Example
  • L (1/G)Lp
  • Lp 100 km
  • L 100 kmv(1-(0.999978)2)
  • L 0.66 km 660 m

15
Relativistic Velocity Addition
  • When objects are moving at relativistic speeds,
    classical mechanics cannot be used.
  • v (v' u) / (1 v'u/c2)
  • v velocity addition
  • v' velocity of object moving in the reference
    frame of u.
  • u motion of object

16
Relativistic Velocity Addition Example
  • A spaceship moving away from Earth at a speed of
    0.80c fires a missile parallel to its direction
    of motion. The missile moves at a speed of 0.60c
    relative to the ship. What is the speed of the
    missile as measured by an observer on Earth?

17
Relativistic Velocity Addition Example
  • Cannot use classical mechanics.
  • v is the velocity we are looking for.
  • u 0.80c the velocity of the spaceship
  • v' 0.60c the velocity of the missile in the
    reference frame of the spaceship
  • v (v' u) / (1 v'u/c2)
  • v (0.6c 0.8c) / (1 (0.6c)(0.8c)/c2)
  • v 1.40c/1.48 0.95c

18
Relativistic Velocity Addition Example
  • A star cruiser is moving away from the planet
    Mars with a speed of 0.58c and fires a rocket
    back towards the planet at a speed of 0.69c as
    seen from the star cruiser. What is the speed of
    the rocket as measured by an observer on the
    planet?

19
Relativistic Velocity Addition Example
  • v is the velocity we are looking for.
  • u 0.58c the velocity of the spaceship
  • v' -0.69c the velocity of the rocket in the
    reference frame of the star cruiser
  • v (v' u) / (1 v'u/c2)
  • v (0.58c - 0.69c) / (1 (0.58c)(-0.69c)/c2)
  • v -0.11c/0.5998 -0.18c
  • Compared to 0.11c

20
Twin Paradox
  • A clock in motion runs slower than one at rest,
    including biological clocks.
  • Apparent paradox with one twin staying on earth
    and other going on a relativistic journey.
  • Solution

21
(No Transcript)
22
Twin Paradox Example
  • Twin sisters Betty and Ann decide to test the
    relativity theory. Ann stays on earth. On
    January 1, 2000, Betty goes off to a nearby dwarf
    star that is 8 light years from Earth. Betty
    travels there and back at 0.8c.

23
Twin Paradox Example
  • What is Bettys travel time to the star according
    to Ann?
  • t d/v 8 light years / 0.8c 10 years
  • So Bettys total travel time according to Ann is
    20 years.

24
Twin Paradox Example
  • As soon as Betty reaches the star, she sends her
    sister an e-mail message saying, Wish you were
    here! via radio. When, from Anns perspective,
    does Ann receive the e-mail from Betty?
  • 2010 8 yrs 2018

25
Twin Paradox Example
  • When Ann receives Bettys e-mail message, what is
    the date on it?
  • Time dilation G 1/v(1- (0.8c)2/c2)
  • So G 0.6c
  • 10 years 0.6c 6 years have passed
  • So the e-mail will have the date of January 2006.

26
Twin Paradox Example
  • How much younger is Betty than Ann when Betty
    returns from the star?
  • For Betty, her return date is 2012, but for Ann,
    she returns in 2020.
  • Ann is now 8 years older than Betty.

27
Twin Paradox Example
28
Newtonian Gravity
  • Quote from Newton
  • Two masses in Newtons theory inertial mass and
    gravitational mass
  • Newton saw no reason why these masses should be
    equal
  • BUT they are!!!

29
Einstein on Gravity
  • I was sitting in a chair in the patent office at
    Bern when all of a sudden a thought occurred to
    me if a person falls freely he will not feel
    his own weight. This simple thought made a deep
    impression on me. It impelled me toward a theory
    of gravitation.
  • -Albert Einstein

30
Principle of Equivalence
  • There is no local experiment that can be done to
    distinguish between the effects of a uniform
    gravitational field in a non-accelerating
    inertial frame and the effects of a uniformly
    accelerating reference frame.

31
Principle of Equivalence
  • Free space view is the same as the free fall view

32
General Relativity
  • The presence of matter causes spacetime to warp
    or curve.
  • Gµv 8?G/c4Tµv

33
Schwarzschilds Solution
  • Found the first exact solution of one of
    Einsteins equations
  • The metric (distance relation) is
  • ds2 -c2(1-2MG/c2r)dt2 dr2/(1-2MG/c2r)
    r2(dq2sin2qdf2).
  • Describes space-time geometry around a spherical
    object of mass M
  • Basis of tests of general relativity

34
Testing the General Theory of Relativity
  • Deflection of Starlight
  • First tested during total solar eclipse in 1919

35
Slowing Down of Clocks by Gravity
  • Clock closer to the mass measures a shorter
    elapsed proper time than a clock that is further
    out.
  • Rc2MG/c2, where Rc is the Schwarzschild radius.
Write a Comment
User Comments (0)
About PowerShow.com