A Harvard pole vaulter carries a pole that is just as long as a barn. He encounters a NJ farmer. Overhead view: Is this Nonsense? -- Space & Time are Relative.

Slides:



Advertisements
Similar presentations
Faster-Than-Light Paradoxes in Special Relativity
Advertisements

Special Relativistic Paradoxes PHYS 206 – Spring 2014.
Relativistic mechanics
O’ O X’ X Z’ Z 5. Consequences of the Lorentz transformation
Lecture 13 Space Time Diagrams ASTR 340 Fall 2006 Dennis Papadopoulos.
Wednesday, October 24: Midterm #1 Material covered: Events, reference frames, spacetime The interval Simultaneity (and relativity thereof) Lorentz transformations.
Lecture Twelve.
Relativistic Paradoxes Physics 11 Adv. Ladder and Barn Paradox A ladder and barn are both measured in the rest frame of the barn; if the barn is shorter.
A lecture series on Relativity Theory and Quantum Mechanics The Relativistic Quantum World University of Maastricht, Sept 24 – Oct 15, 2014 Marcel Merk.
LECTURE 5 SPACE-TIME DIAGRAMS PHYS 420-SPRING 2006 Dennis Papadopoulos.
Theory of Relativity Albert Einstein Physics 100 Chapt 18.
Modern Physics (PC300) Class #5 Cool, but not as fast as we are talking about! Notes: Test a week from Tuesday Old tests are avail. Homework due Wednesday.
The laws of physics are the same in any inertial (non- accelerating) frame of reference Galileo & Einstein would both agree (at terrestrial speeds.) F=ma.
Two balloons sit on the physics lecture hall desk, at the left and right edges. The balloon at the left edge bursts, and 2 seconds later the balloon at.
EPPT M2 INTRODUCTION TO RELATIVITY K Young, Physics Department, CUHK  The Chinese University of Hong Kong.
Special Relativity & General Relativity
Special Relativity. Topics Motion is Relative Michelson-Morley Experiment Postulates of the Special Theory of Relativity Simultaneity Spacetime Time Dilation.
4-vectors: Four components that Lorentz transform like ct, x, y, z.
Causality in special relativity
Lecture 14 Space-time diagrams (cont) ASTR 340 Fall 2006 Dennis Papadopoulos.
PH 301 Dr. Cecilia Vogel Lecture 5. Review Outline  Velocity transformation  NOT simple addition  Spacetime  intervals, diagrams  Lorentz transformations.
Further Logistical Consequences of Einstein’s Postulates
Special Relativity The Death of Newtonian Physics.
The Four Dimensional World Spacetime: a piece of Einstein’s General Theory of Relativity.
© 2010 Pearson Education, Inc. Chapter S3 Spacetime and Gravity.
You may pick up your R1 and R2 problems on the front desk. There are 5 points possible on each. The solutions are on-line, password is PH365. R3 problems.
TWO BASIC RESULTS Time dilation  t(v) = [1/(1 – v 2 /c 2 ) 1/2 ]  t(0) Length Contraction d(v) = (1 – v 2 /c 2 ) 1/2 d(0)
Special Theory of Relativity
Chapter R2 Synchronizing Clocks. Newtonian time Time was held to be universal. Clocks ran the same in all inertial systems. In these systems if one system.
Einstein’s postulates 1.The laws of nature are the same for everyone. 2. The speed of light in a vacuum is constant for all observers.
1 1.Einstein’s special relativity 2.Events and space-time in Relativity 3. Proper time and the invariant interval 4. Lorentz transformation 5. Consequences.
Tue. Jan. 6 – Physics Lecture #17 Relativity – SpaceTime 1) Invariants & Spacetime interval 2) Time-like, Light-like, Space-like intervals 3) Spacetime.
Little drops of water, little grains of sand, make the mighty ocean and the pleasant land. Little minutes, small though they may be, make the mighty ages.
Special Relativity The Failure of Galilean Transformations
It’s all Relativity. March, 1905: Twenty six year old Albert Einstein demonstrates the particle nature of light by explaining the photoelectric effect.
1 1.Einstein’s special relativity 2.Events and space-time in Relativity 3. Proper time and the invariant interval 4.Lorentz transformation Einstein’s special.
Special Theory of Relativity Einstein pondered the question, “If I could ride a beam of light, what would I see?” Meaning, if a car moved at the speed.
Physics 2170 – Spring Special relativity Homework solutions are on CULearn Remember problem solving sessions.
Modern Physics (PC300) Class #3 Moore - Chapter R3 - Time Chapter R4 - Metric Equation Chapter R5 – Proper time Chapter R6 – Coordinate Transformations.
Modern Physics (PC301) Class #4 Moore - Chapter R5 – Proper time
Wed., Sept. 12, 2012PHYS , Fall 2012 Dr. Jaehoon Yu 1 PHYS 3313 – Section 001 Lecture #5 Wednesday, Sept. 12, 2012 Dr. Jaehoon Yu Spacetime Diagram&
SYNTHESIS Space-Time Revisited 1.Antimatter 2.Feynman Diagrams 3.Quantum Electrodynamics.
Physics 102: Lecture 28, Slide 1 Special Relativity Physics 102: Lecture 28 Make sure your grade book entries are correct Bring ID to Final EXAM!!!! Today’s.
The Twin Paradox Brenda goes off at 4/5 c to a distant star and then returns. Her twin brother Ali stays on Earth. When she gets back she is no longer.
Advanced EM - Master in Physics X (m) Time (m) O B Every “trajectory in spacetime”, such as the two drawn in the figure, is called a worldline.
When ready, begin the Slide Show on this slide. To progress through a slide, press the down arrow or right arrow key. To go back, press the up or left.
 The laws of physics must be the same in all inertial reference frames  The speed of light in vacuum has the same value in all inertial frames, regardless.
1 1.Time Dilation 2.Length Contraction 3. Velocity transformation Einstein’s special relativity: consequences.
4.4 Images in a Plane Mirror. Images in Plane Mirrors When you place an object in front of a mirror the light rays reflect off the object and some will.
Einstein’s Second Revolution. Movement on the surface of the Earth is limited to two dimensions: forward-backward and left-right (or N-S and E-W) However,
Time Dilation. Relative Time  Special relativity predicts that events seen as simultaneous by one observer are not simultaneous to an observer in motion.
Special Relativity Lecture 25 F2013 Lorentz transformations 1.
Causality in special relativity
Problem: A rocket travels away from earth at constant speed v to planet Q. The trip takes 100 years, as measured on earth but only 25 years as measured.
 The laws of mechanics must be the same in all inertial reference frames  Time is the same across all reference frames  Simple addition of velocities.
4-vectors: Four components that Lorentz transform like ct, x, y, z.
Chapter S3 Spacetime and Gravity
PHYS 3313 – Section 001 Lecture #8
Harrison B. Prosper Florida State University YSP
PHYS 3313 – Section 001 Lecture #6
Wacky Implications of Relativity
Special Relativity.
Albert Einstein and 100 Years of Relativity
Given eqns Also P4.
A New Vision of the Cosmos
Special relativity: energy, momentum and mass
Aim: How do we explain the special theory of relativity?
Spacetime Structure.
PHYS 3313 – Section 001 Lecture #8
Principle of Equivalence: Einstein 1907
Presentation transcript:

A Harvard pole vaulter carries a pole that is just as long as a barn. He encounters a NJ farmer. Overhead view: Is this Nonsense? -- Space & Time are Relative

The farmer gathers 100 witnesses and this is what they see: The pole vaulter then bursts through the second door. The witnesses ALL agree: THE FARMER WON

? According to the Pole Vaulter, the Farmer cheats!! He shuts the front door before the back one! But, alas, not one witness agrees

A New Geometry for Space and Time Space, Time, Simultaneity, Energy, Momentum are all relative Yet, some things, like the speed of light, are absolutes (“invariants”)

ct x SPACE-TIME DIAGRAM WELCOME TO YOUR 4-DIMENSIONAL WORLD Bob’s viewpoint

ct x SPACE-TIME DIAGRAM an event a worldline light

y x SPACE-SPACE DIAGRAM a point

y x SPACE-SPACE DIAGRAM y’y’ x’x’ a point

ct SPACE-TIME DIAGRAM light x Bob’s viewpoint

ct SPACE-TIME DIAGRAM light ct ’ x x’x’ Alice’s viewpoint

ct SPACE-TIME DIAGRAM light ct ’ x x’x’

ct SPACE-TIME DIAGRAM ct ’ x x’x’ an event

ct SPACE-TIME DIAGRAM ct ’ x x’x’ an event

ct TIME & SIMULTANEITY ARE RELATIVE x Farmer’s viewpoint

ct ct ’ x x’x’ TIME & SIMULTANEITY ARE RELATIVE first second Pole vaulter’s viewpoint

Alice Bob people “Twin Paradox” Revisited v Alice Bob v The End ?

t x AT LAST: THE TWIN PARADOX Alice takes off Alice returns

t x SPACE-TIME DIAGRAM Alice takes off Alice returns Bob’s “worldline”

t x SPACE-TIME DIAGRAM Alice takes off Alice returns Alice’s “worldline” Kink: only Alice feels acceleration

y x SPACE-SPACE DIAGRAM Shortest distance between two points is a straight line

t x SPACE-TIME DIAGRAM Alice takes off Alice returns Alice’s “worldline” Longest time between two events is a straight line

E = mc 2 E =  m rest c 2