Relativity IV Non-rel. Modern Art Quiz Lorentz Transformations

Slides:



Advertisements
Similar presentations
Classical Relativity Galilean Transformations
Advertisements

Cutnell/Johnson Physics 7th edition
Derivation of Lorentz Transformations
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.
Special Theory of Relativity
Life in the fast lane: the kinematics of Star Trek.
Copyright © 2012 Pearson Education Inc. PowerPoint ® Lectures for University Physics, Thirteenth Edition – Hugh D. Young and Roger A. Freedman Lectures.
Special Relativity & General Relativity
Special Relativity. Topics Motion is Relative Michelson-Morley Experiment Postulates of the Special Theory of Relativity Simultaneity Spacetime Time Dilation.
Life in the fast lane: the kinematics of Star Trek.
1 PH300 Modern Physics SP11 1/27 Day 5: Questions? Time Dilation Length Contraction Next Week: Spacetime Relativistic Momentum & Energy “I sometimes ask.
2. Einstein's postulates in special theory of relativity
Announcements Homework: Supplemental Problems 2 nd Project is due at the final exam which is Tuesday May 5 at 1:30 – 3:30pm. A list of potential projects.
A lecture series on Relativity Theory and Quantum Mechanics The Relativistic Quantum World University of Maastricht, Sept 24 – Oct 15, 2014 Marcel Merk.
Introduction to special relativity
Page 1 Phys Baski Relativity I Topic #9: Special Relativity I Transformation of Variables between Reference Frames –Non-relativistic Galilean Transformation.
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.
Chapter 28 Special Relativity Events and Inertial Reference Frames An event is a physical “happening” that occurs at a certain place and time. To.
Education Physics Deparment UNS
The Theory of Special Relativity. Learning Objectives  Einstein’s two postulates in his theory of special relativity: The principle of relativity. (Same.
My Chapter 26 Lecture.
Consequences of Special Relativity Simultaneity: Newton’s mechanics ”a universal time scale exists that is the same for all observers” Einstein: “No universal.
Physics 2170 – Spring Special relativity Homework solutions will be on CULearn by 5pm today. Next weeks.
Special relativity Part II Recall Einstein’s Postulates (1905) First Postulate –The laws of physics are the same in any inertial frame of reference (principle.
Chapter 39 Relativity. A Brief Overview of Modern Physics 20 th Century revolution 1900 Max Planck Basic ideas leading to Quantum theory 1905 Einstein.
11.1 – Frames of Reference and Relativity
Derivation of Lorentz Transformations Use the fixed system K and the moving system K’ At t = 0 the origins and axes of both systems are coincident with.
Special Theory of Relativity. Galilean-Newtonian Relativity.
Galileo’s Relativity: Text: The laws of mechanics are the same in all inertial reference frames. More general: The laws of mechanics are the same in all.
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,
By: Jennifer Doran. What was Known in 1900 Newton’s laws of motion Maxwell’s laws of electromagnetism.
Special Relativity (Math)  Reference from Tipler chapter 39-1 to 39-3  Newtonian relativity  Einstein’s postulates  Lorentz transformation  Time dilation.
PHYS 342: More info The TA is Meng-Lin Wu: His is His office hour is 10:30am to 12pm on Mondays His office is Physics.
Chapter 28 Special Relativity Events and Inertial Reference Frames An event is a physical “happening” that occurs at a certain place and time. To.
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.
Relativity Part III If twin Astrid aged 10 years during her high-speed trip and Eartha aged 50 years, what is gamma ? What is u ? Ans: γ=5, u~0.980c Twin.
Some places where Special Relativity is needed
RELATIVITY.
Special Relativity I Today: Quiz Special Relativity
Life in the fast lane: the kinematics of Star Trek
English translation of the original (not so different from the textbook). English translation of Einstein’s 1905 paper on special relativity
Administrative Details: PHYS 344
Chapter S2 Space and Time
Special Relativity II Two-minute movie Quiz Breakdown of simultaneity
History: Special Relativity‘s impact on 20th century art
The Relativistic Quantum World
Physics: Principles with Applications, 6th edition
Physics 6C Special Relativity Prepared by Vince Zaccone
Wacky Implications 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,
Classical Physics “Inertial Reference Frame” (Section 5.2):
Special Relativity Speed of light is constant Time dilation
Einstein’s Relativity Part 2
Michelson-Morley Developed an experiment to measure the speed of light in different directions Ether was the assumed medium in which light waves traveled.
Special Relativity Lecture 2 12/3/2018 Physics 222.
An Introduction To ‘High Speed’ Physics
Chapter 28: Special Relativity
Announcements Apologies: Karen Mertz and Prof. Szarmes sent in an order for the PHYS274 text book over three months ago. The Hawaii representative of.
Special relativity Physics 123 1/16/2019 Lecture VIII.
The Galilean Transformations
RELATIVITY III SPECIAL THEORY OF RELATIVITY
The Galilean Transformation
PHYS 3700 Modern Physics Prerequisites: PHYS 1212, MATH Useful to have PHYS 3900 or MATH 2700 (ordinary differential equations) as co-requisite,
Key Areas covered The speed of light in a vacuum is the same for all observers. The constancy of the speed of light led Einstein to postulate that measurements.
Special Relativity Chapter 1-Class3.
Lorentz Transformations
Chapter 37 Special Relativity
Special Relativity Chapter 1-Class4.
Presentation transcript:

Relativity IV Non-rel. Modern Art Quiz Lorentz Transformations Relativistic addition of velocities Doppler Effect

History: Special Relativity‘s apparent impact on 20th century art   “In the intellectual atmosphere of 1905 it is not surprising that Einstein and Picasso began exploring new notions of space and time almost coincidentally.….Just as relativity theory overthrew the absolute status of space and time, the cubism of Georges Braque and Picasso dethroned perspective in art.” Anyone want to guess what this is a picture of? Galison et al disputes this claim. Georges Braque, Man with Guitar 2

Special Relativity‘s possible impact on 20th century art Ans: Salvador Dali. 1931 “The persistence of memory.” Who was the artist ? 3

Suppose we have a space ship capable of traveling at 0.5c. Q11.1 Suppose we have a space ship capable of traveling at 0.5c. An astronaut travels to a destination 1 light-year from Earth. When she reaches there, how much time has elapsed according to her clock on the spaceship? D (delta t_0 = delta t/gamma); 0.5**2=0.25 4

Suppose we have a space ship capable of traveling at 0.5c. Q11.1 Suppose we have a space ship capable of traveling at 0.5c. An astronaut travels to a destination 1 light-year from Earth. When she reaches there, how much time has elapsed according to her clock on the spaceship? Takes 2 years to travel 1 light year at 0.5c in frame S D (delta t_0 = delta t/gamma); 0.5**2=0.25 β = 0.5; β2 = 0.25 Δt0 = Δt/γ 5

Q11.2 A crewman measures the length his space ship to be 50 meters long. The space ship passes by Earth at 0.8c with respect to Earth. What is the length of the spaceship according to an observer on Earth ? 50 m 60 m 30 m 23 m C (Lorentz contraction L = L_0/gamma = 50m/gamma gamma=1/sqrt(1-0.8**2)=1.66 50m/1.66=30m 6

Q11.2 A crewman measures the length his space ship to be 50 meters long. The space ship passes by Earth at 0.8c with respect to Earth. What is the length of the spaceship according to an observer on Earth ? 50 m 60 m 30 m 23 m Length contraction 50m/1.66 = 30m C (Lorentz contraction L = L_0/gamma = 50m/gamma gamma=1/sqrt(1-0.8**2)=1.66 50m/1.66=30m γ = 1/sqrt(1-0.8**2) = 1.66 7

Q11.3 A 8

Remember, if one transforms to x,t coordinates, velocity changes sign Q11.3 A Remember, if one transforms to x,t coordinates, velocity changes sign 9

Q11.4 B 10

Q11.4 B 11

The Lorentz transformations Lorentz transformations relate the coordinates and velocities in two inertial reference frames. They are more general than the Galilean transformations and are consistent with the principle of relativity. Galilean transformations. Do not work at relativistic velocities. 12

The Lorentz transformations (“boost along x”) Space and time are intertwined: 4 dimensional “space-time” Intellectual revolution Note the coordinates perpendicular to the “boost“ are unmodified Check the s(i)gn. 13

The Lorentz transformations (“boost along x”) Space and time are intertwined: 4 dimensional “space-time” Intellectual revolution. Note the two equations are related. Time dilation Caution! Don’t confuse these 2 !! 14

How do we calculate a “relativistic boost along y” ? Note the coordinates perpendicular to the “boost“ are unmodified 15

Example using the Lorentz transformations Winning an interstellar race, Mavis pilots her spaceship across a finish line in space at a speed of 0.600 c. A “hooray” message is sent from the back of her ship (event 2) at the instant in her frame of reference that the front of her ship crosses the finish line (event 1). Mavis measures the length of her ship to be 300 m. Stanley is located at the finish line and is at rest relative to it. When and where does Stanley measure events 1 and 2 to occur ? S is Stanley’s frame while S’ is Mavis’ frame Event 1 occurs at x=0, t=0 in S and x’=t’=0 in S’ Event 2 in S’ (Mavis’ frame) occurs at t’=0, x’=-300m Let’s use the Lorentz transformation to find x and t in Stanley’s frame 16

Example using the Lorentz transformations S is Stanley’s frame while S’ is Mavis’ frame Event 1 occurs at x=0, t=0 in S and x’=t’=0 in S’ Event 2 in S’ (Mavis’ frame) occurs at t’=0, x’=-300m Let’s use the Lorentz transformation to find x and t in Stanley’s frame [but be careful, let’s change x’ x, t’t and therefore u(-u)] Note that in Mavis’ frame the two events are simultaneous (so simultaneity has broken down in this example). Note that in Mavis’ frame the two events are simultaneous (so simultaneity has broken down in this example). 17

Relativistic addition of velocities (take differentials) Start from Lorentz transformations. 18

Relativistic addition of velocities cont’d This gives velocities in S’ in terms of S where S’ is moving at velocity u with respect to S. Question: How do we get velocities in S in terms of velocities in S’ ? Ans: interchange primed and unprimed velocities and change u to –u (why ?) 19

Relativistic addition of velocities Question: What happens if vx=c ? Ans: vx’=c (according to Einstein’s second postulate). Let’s check if this really works ✔ Question: what happens if u<<c ? 20

Relativistic addition of velocities example (part a) A spaceship moving away from earth at 0.900c fires a robot probe at 0.700c relative to the spaceship. What is the probe’s velocity relative to the earth ? Let S and S’ be the reference frames of the Earth and the Spaceship. Their relative velocity of S’ and S are u=0.900c. Note the sgn I get v_x= 0.9816 21

Relativistic addition of velocities example (part b) A scoutship is sent to catch up at 0.950 relative to the earth. What is the velocity of the scoutship relative to the spaceship ? Let S and S’ be the reference frames of the Scoutship and the Spaceship. Their relative velocity of S’ and S are u=0.900c. Note the sgn I get 0.3448c 22

Bank Robbery! The notorious intergalactic bank robbers, known as the Warp Drive Kids, has hit the First Alpha Centari bank, and is trying to make a getaway. They are cruising to the Dark Sector at their maximum speed of 0.8c Fortunately a police star cruiser was already en route to the Dark Sector at its maximum speed of 0.3c. Therefore it launched an interceptor at 0.6c. Assuming both start equidistant from the Dark Sector, will intercept happen before the bad guys can go dark? I get v_x= 0.9816 According to Galileo? Yes No Dead heat Impossible to know 23

Bank Robbery! The notorious intergalactic bank robbers, known as the Warp Drive Kids, has hit the First Alpha Centari bank, and is trying to make a getaway. They are cruising to the Dark Sector at their maximum speed of 0.8c Fortunately a police star cruiser was already en route to the Dark Sector at its maximum speed of 0.3c. Therefore it launched an interceptor at 0.6c. Assuming both start equidistant from the Dark Sector, will intercept happen before the bad guys can go dark? I get v_x= 0.9816 According to Galileo? Yes No Dead heat Impossible to know 0.6c+0.3c = 0.9c 24

Bank Robbery! The notorious intergalactic bank robbers, known as the Warp Drive Kids, has hit the First Alpha Centari bank, and is trying to make a getaway. They are cruising to the Dark Sector at their maximum speed of 0.8c Fortunately a police star cruiser was already en route to the Dark Sector at its maximum speed of 0.3c. Therefore it launched an interceptor at 0.6c. Assuming both start equidistant from the Dark Sector, will intercept happen before the bad guys can go dark? I get v_x= 0.9816 According to Einstein? Yes No Dead heat 25

Bank Robbery! The notorious intergalactic bank robbers, known as the Warp Drive Kids, has hit the First Alpha Centari bank, and is trying to make a getaway. They are cruising to the Dark Sector at their maximum speed of 0.8c Fortunately a police star cruiser was already en route to the Dark Sector at its maximum speed of 0.3c. Therefore it launched an interceptor at 0.6c. Assuming both start equidistant from the Dark Sector, will intercept happen before the bad guys can go dark? I get v_x= 0.9816 Vtotal = u+vintercept/(1+u.vintercept) Yes No Dead heat Vtotal = 0.76c Vtotal = (0.3c)+(0.6c)/(1+ (0.3c).(0.6c)) 26

Salzburg, Austria Read 37.9 General Relativity