About length contraction Moving bodies are short.

Slides:



Advertisements
Similar presentations
Einsteins Special Theory of Relativity. Relative Motion ALL motion is relative Speeds are only measured in relation to other objects No way to determine.
Advertisements

Special Relativistic Paradoxes PHYS 206 – Spring 2014.
Relativistic mechanics
Lecture 20 Relativistic Effects Chapter Outline Relativity of Time Time Dilation Length Contraction Relativistic Momentum and Addition of Velocities.
Building Spacetime Diagrams PHYS 206 – Spring 2014.
Physics Lecture Resources
relativity Quantum Classic physics Modern physics.
M. Cobal, PIF 2006/7 Units and kinematics. M. Cobal, PIF 2006/7 Units in particle physics.
Lecture Twelve.
1 Special Relativity 2. 2 Topics l Recap l Length Contraction l Cosmic Ray Muons l Spacetime l Summary.
Phy107 Fall 2006 From last time… Einstein’s Relativity ◦ All laws of physics identical in inertial ref. frames ◦ Speed of light=c in all inertial ref.
Physics 3 for Electrical Engineering Ben Gurion University of the Negev
Special Relativity Lecture 24 F2013 The Postulates Phenomenology The proper frame Time Length Mass energy Measuring events Lorentz transformations 1.
Physics 311 Special Relativity Lecture 5: Invariance of the interval. Lorentz transformations. OUTLINE Invariance of the interval – a proof Derivation.
Lorentz Transformation
1 Length contraction Length measured differs from frame to frame – another consequence of relativistic effect Gedankan experiment again!
Principle of special relativity Their is inconsistency between EM and Newtonian mechanics, as discussed earlier Einstein proposed SR to restore the inconsistency.
EPPT M2 INTRODUCTION TO RELATIVITY K Young, Physics Department, CUHK  The Chinese University of Hong Kong.
PHY 1371Dr. Jie Zou1 Chapter 39 Relativity (Cont.)
Homework #3 L-8 (25 points) L-16 (25 points) 4-1 (20 points) Extra credit problem (30 points): Show that Lorentz transformations of 4-vectors are similar.
Chapter 37 Special Relativity. 37.2: The postulates: The Michelson-Morley experiment Validity of Maxwell’s equations.
Time Dilation, Length Contraction and Doppler
1 Tutorial Reminder Please download the tutorial from the course web page and try them out Tutorial class will be conducted on 12 DEC 03 (Friday) Submit.
Relativistic Velocity. Galilean Transformation  Relative velocity has been used since the time of Galileo. Sum velocity vectorsSum velocity vectors Relative.
IB Physics – Relativity Relativity Lesson 2 1.Time dilation 2.Lorentz Factor 3.Proper time 4.Lorentz contraction 5.Proper length 6.Twin paradox and symmetric.
The Lorentz Transformation Section 4. An event has coordinates x,y,z,t in the K system x’,y’,z’,t’ in the K’ system What is the formula that transforms.
Introduction to special relativity
Special Theory of Relativity
Special relativity.
Special Relativity Space and Time. Spacetime Motion in space is related to motion in time. Special theory of relativity: describes how time is affected.
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.
Special Relativity: “all motion is relative”
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.
1 PHYS 3313 – Section 001 Lecture #5 Wednesday, Jan. 29, 2014 Dr. Jaehoon Yu Length Contraction Relativistic Velocity Addition The Twin Paradox Space-time.
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.
Time Dilation We can illustrate the fact that observers in different inertial frames may measure different time intervals between a pair of events by considering.
Consequences of Lorentz Transformation. Bob’s reference frame: The distance measured by the spacecraft is shorter Sally’s reference frame: Sally Bob.
Physics 2170 – Spring Special relativity Homework solutions are on CULearn Remember problem solving sessions.
Chapter 28: Special Relativity
Modern Physics Relativity 1 Space is defined by measurements of length and depends on what “ruler” is used to measure the length. Time is defined by measurements.
My Chapter 26 Lecture.
Introduction Classical Physics Laws: Mechanics (Newton), Electromagnetism (Maxwell), Optics, Fluids,.. Etc. Modern Physics: What do we mean? Are the laws.
1 Relativity  H3: Relativistic kinematics  Time dilation  Length contraction.
Module 10Energy1 Module 10 Energy We start this module by looking at another collision in our two inertial frames. Last time we considered a perfectly.
Consequences of Special Relativity Simultaneity: Newton’s mechanics ”a universal time scale exists that is the same for all observers” Einstein: “No universal.
Length Contraction. Relative Space  An observer at rest measures a proper time for a clock in the same frame of reference.  An object also has a proper.
SPECIAL THEORY OF RELATIVITY. Inertial frame Fig1. Frame S’ moves in the +x direction with the speed v relative to frame S.
Special Theory of Relativity. Galilean-Newtonian Relativity.
Special Relativity Lecture 25 F2013 Lorentz transformations 1.
Relativity Questions Chris Parkes. Motion As a high-speed spaceship flies past you at half the speed of light, it fires a strobe light. An observer on.
Lecture 5: PHYS344 Homework #1 Due in class Wednesday, Sept 9 th Read Chapters 1 and 2 of Krane, Modern Physics Problems: Chapter 2: 3, 5, 7, 8, 10, 14,
Lorentz Transformation and Lorentz Contraction The analytical centerpiece.
Lecture 13.
Special Theory of Relativity
PHYS 3313 – Section 001 Lecture #6
Quiz_09 Relativity – simultaneity, time dilation, length contraction
Lecture 4: PHYS 344 Homework #1 Due in class Wednesday, Sept 9th Read Chapters 1 and 2 of Krane, Modern Physics Problems: Chapter 2: 3, 5, 7, 8, 10, 14,
پروتكل آموزش سلامت به مددجو
Newtonian Relativity A reference frame in which Newton’s laws are valid is called an inertial frame Newtonian principle of relativity or Galilean invariance.
Einstein’s Relativity Part 2
…understanding momentum in spacetime
Special Relativity Lecture 2 12/3/2018 Physics 222.
Chapter 28: Special Relativity
The Galilean Transformations
The Galilean Transformations
Relativistic Kinematics
Chapter 37 Special Relativity
Special Relativity Chapter 1-Class4.
Time dilation recap: A rocket travels at 0.75c and covers a total distance of 15 light years. Answer the following questions, explaining your reasoning:
Presentation transcript:

About length contraction Moving bodies are short

How can we measure the length of a moving body?

If (x 1 ;t) and (x 2 ;t) are the space-time coordinates of such events, then the length of the body is given by = |x 2 – x 1 | =  x What’s the relationship with the length of the body according to a reference frame in which the body is at rest (this length being called “proper length”).

A simple answer can be found by applying Lorentz’s transformation to the coordinates of the two events. From:x’ =  (x – V  t)we get:  x’ =  (  x – V  t). As  t = 0 and  x =, we finally get: where a contraction along the direction of motion is found, being  > 1.

Another way to get this result

What’s the relationship with the body’s length according to a reference frame in which the body is at rest?

 t’ is related to  t 0 by the time dilation law  t’ =  t 0 So, again, we get: