PHYS-3301 Lecture 5. Chapter 2. Announcement. Sep. 12, Special Relativity. What about y and z coordinates? (x - direction of motion)

Size: px
Start display at page:

Download "PHYS-3301 Lecture 5. Chapter 2. Announcement. Sep. 12, Special Relativity. What about y and z coordinates? (x - direction of motion)"

Transcription

1 Announemen Course webpage hp:// Tebook PHYS-33 Leure 5 HW (due 9/4) Chaper, 6, 36, 4, 45, 5, 5, 55, 58 Sep., 7 Chaper Speial Relaiiy. Basi Ideas. Consequenes of Einsein s Posulaes 3. The Lorenz Transformaion Equaions 4. The Twin Parado 5. The Doppler Effes 6. Veloiy Transformaion 7. Momenum Energy 8. General Relaiiy a s Look a Cosmology 9. The Ligh Barrier. The 4 h Dimension Wha abou y and z oordinaes? ( - direion of moion)

2 Doppler Effe Parallel o he Direion of Relaie moion Orhogonal o he Direion of Relaie moion Relaiisi Dynamis Epressions for (oal) Energy and Momenum of a parile of mass m, moing a eloiy u Ouline: Relaiisi Momenum Relaiisi Kinei Energy Toal Energy Momenum and Energy in Relaiisi Mehanis General Theory of Relaiiy Ne Week Quanum Physis

3 E INTERNAL ENERGY E INTERNAL m Kinei Energy KE E TOTAL ENERGY E p (m ) u u

4 u Is here Absolue Causaliy? Migh ause preede effe in one referene frame bu effe preede ause in differen referene frame(s)? e.g. an someone see you firs die, and hen see you ge born? Is here Absolue Causaliy? Le s assume ha he order of eens is hanged in some referene frame S Migh ause preede effe in one referene frame bu effe preede ause in differen referene frame(s)? e.g. an someone see you firs die, and hen see you ge born? Is ha Possible? and are he ime inerals beween he same wo eens obsered in S and S, respeiely

5 Le s assume ha he order of eens is hanged in some referene frame S Is ha Possible? and are he ime inerals beween he same wo eens obsered in S and S, respeiely Using Lorenz ransformaions. if hen Using Lorenz ransformaions. if hen Using Lorenz ransformaions. if hen Impossible??

6 Is here Absolue Causaliy? YES Migh ause preede effe in one referene frame bu effe preede ause in differen referene frame(s)? NO Relaiisi Dynamis Some Eamples e.g. an someone see you firs die, and hen see you ge born? NO s. Wha is he momenum of an eleron wih K m? s. Wha is he momenum of an eleron wih K m? 4 E p m E m K p m m 4m m 3m. How fas is a proon raeling if is kinei energy is /3 of is oal energy?. How fas is a proon raeling if is kinei energy is /3 of is oal energy? K E ( m K) E 3m 3 3 m E V / ( ) V 8 3 V / 9 3 ( V )

7 An eleron iniially moing wih momenum pm is passed hrough a rearding poenial differene of V ols whih slows i down; i ends up wih is final momenum being m/. (a) Calulae V in ols. (b) Wha would V hae o be in order o bring he eleron o res? An eleron iniially moing wih momenum pm is passed hrough a rearding poenial differene of V ols whih slows i down; i ends up wih is final momenum being m/. (a) Calulae V in ols. (b) Wha would V hae o be in order o bring he eleron o res? (a) E p m m m m pm: ( ) ( ) ( ) Thus, he rearding poenial differene 5 pm/: E m ( m ) m Δ E E E m.3m.3(.5 ev).5 ev (b) ( ) 5 V.5 V E m E m Δ E m. 5 ev V. 5 V The kinemai energy of a proon is half is inernal energy. (a) Wha is he proon s speed? (b) Wha is is oal energy? () Deermine he poenial differene V hrough whih he proon would hae o be aeleraed o aain his speed. An unsable parile of mass m moing wih eloiy relaie o an inerial lab RF disinegraes ino wo gamma-ray phoons. The firs phoon has energy 8 MeV in he lab RF and raels in he same direion as he iniial parile; he seond phoon has energy 4 MeV and raels in he direion opposie o ha of he firs. Wrie he relaiisi equaions for onseraion of momenum and energy and use he daa gien o find he eloiy and res energy, in MeV, of he unsable parile. phoon phoon before afer

8 An unsable parile of mass m moing wih eloiy relaie o an inerial lab RF disinegraes ino wo gamma-ray phoons. The firs phoon has energy 8 MeV in he lab RF and raels in he same direion as he iniial parile; he seond phoon has energy 4 MeV and raels in he direion opposie o ha of he firs. Wrie he relaiisi equaions for onseraion of momenum and energy and use he daa gien o find he eloiy and res energy, in MeV, of he unsable parile. (a) (b) before m ( ) / m ( ) / phoon afer phoon ph ph m ( ) / m ( ) / E E ph ph E E ph ph E E 8MeV 4MeV 4MeV E E 8MeV 4MeV MeV ph ph ( ph ph ) ( ) ( ) momenum onseraion energy onseraion ( a) 4 () b 3 m E E MeV MeV / /9.3 A moing eleron ollides wih a saionary eleron and an eleron-posiron pair omes ino being as a resul. When all four pariles hae he same eloiy afer he ollision, he kinei energy required for his proess is a minimum. Use a relaiisi alulaion o show ha K min 6m, where m is he eleron mass. p 4 p E m 4E energy onseraion before ( ) ( ) ( ) ( ) E m p E m p E m 4E p 4p In he ener-of-mass RF: p before afer p 4p momenum onseraion 6 ( ) ( ) E Em m 6( E ) 6 ( m ) ( p) afer ( m ) ( ) p ( ) ( E) ( p ) Em ( m ) 6( m ) E 4 m / m 7m E 4m E γ m ( m ) ( ) 3 4 V / 3/ K E m m 6 γ ( 48/49) relaie speed V m K m m 6 General Relaiiy General Relaiiy General relaiiy is he geomeri heory of graiaion published by Alber Einsein in 96. Many prediions of general relaiiy differ signifianly from hose of lassial physis. I is he urren desripion of graiaion in modern physis. I unifies speial relaiiy and Newon s law of uniersal graiaion, and desribes graiy as a geomeri propery of spae and ime. In pariular, he uraure of spae-ime is direly relaed o he fourmomenum (mass-energy and momenum). The relaion is speified by he Einsein s field equaions, a sysem of parial differenial equaions (graduae leel ourse). Eamples of suh differenes inlude graiaional ime dilaion, he graiaional red-shif of ligh, and he graiaional ime delay. General relaiiys prediions hae been onfirmed in all obseraions and eperimens o dae. Howeer, unanswered quesions remain, soluion is he quanum graiy sounds quie ompliae..

Doppler Effect. PHYS-2402 Lecture 6. Chapter 2. Announcement. Feb. 3, Special Relativity. Quiz 1: Thursday 30 min; Chap.2

Doppler Effect. PHYS-2402 Lecture 6. Chapter 2. Announcement. Feb. 3, Special Relativity. Quiz 1: Thursday 30 min; Chap.2 Announemen Course webpage hp://highenergy.phys.u.edu/~slee/40/ Tebook PHYS-40 Leure 6 Quiz : Thursday 30 min; Chap. Feb. 3, 05 HW (due /0) 0, 6, 36, 4, 46, 5, 55, 70, 76, 87, 9, Doppler Effe Chaper Speial

More information

2.3 The Lorentz Transformation Eq.

2.3 The Lorentz Transformation Eq. Announemen Course webage h://highenergy.hys.u.edu/~slee/4/ Tebook PHYS-4 Leure 4 HW (due 9/3 Chaer, 6, 36, 4, 45, 5, 5, 55, 58 Se. 8, 6.3 The Lorenz Transformaion q. We an use γ o wrie our ransformaions.

More information

Relativistic Dynamics

Relativistic Dynamics Announemen Course webage h://highenergy.hys.u.edu/~slee/4/ Tebook PHYS-4 Leure Se., 5 Leure Noes, HW Assignmens, Physis Colloquium, e.. Relaiisi Dynamis Chaer Seial Relaiiy. Basi Ideas. Consequenes of

More information

Announcements. Lecture 6 Chapter. 2 Special Relativity. Relativistic Dynamics. Relativistic Kinetic Energy. Relativistic Momentum

Announcements. Lecture 6 Chapter. 2 Special Relativity. Relativistic Dynamics. Relativistic Kinetic Energy. Relativistic Momentum Announemens HW: Ch.-70, 75, 76, 87, 9, 97, 99, 104, 111 HW1 due: now, HW due: /08 (by lass hour) No lab his week; New TA (Ganga) Physis Colloquium (Thursday a 3:40m) Quiz 1: Feb 8 h. (30 min) -- Cha. ***

More information

The Special Theory of Relativity Chapter II

The Special Theory of Relativity Chapter II The Speial Theory of Relaiiy Chaper II 1. Relaiisi Kinemais. Time dilaion and spae rael 3. Lengh onraion 4. Lorenz ransformaions 5. Paradoes? Simulaneiy/Relaiiy If one obserer sees he eens as simulaneous,

More information

Generalized The General Relativity Using Generalized Lorentz Transformation

Generalized The General Relativity Using Generalized Lorentz Transformation P P P P IJISET - Inernaional Journal of Innoaie Siene, Engineering & Tehnology, Vol. 3 Issue 4, April 6. www.ijise.om ISSN 348 7968 Generalized The General Relaiiy Using Generalized Lorenz Transformaion

More information

Chapter 1 Relativity

Chapter 1 Relativity Chaper Relaii - Posulaes of Speial Relaii and Loren Transformaion The s posulae: The laws of phsis ma be epressed in equaions haing he same form in all frames of referene moing a onsan eloi wih respe o

More information

Mocanu Paradox of Different Types of Lorentz Transformations

Mocanu Paradox of Different Types of Lorentz Transformations Page Moanu Parado of Differen Types of Lorenz Transformaions A R aizid and M S Alam * Deparmen of usiness Adminisraion Leading niersiy Sylhe 300 angladesh Deparmen of Physis Shahjalal niersiy of Siene

More information

Newtonian Relativity

Newtonian Relativity Newonian Relaii A referene frame in whih Newon s laws are alid is alled an inerial frame Newonian priniple of relaii or Galilean inariane If Newon s laws are alid in one referene frame, hen he are also

More information

Can you guess. 1/18/2016. Classical Relativity: Reference Frames. a x = a x

Can you guess. 1/18/2016. Classical Relativity: Reference Frames. a x = a x /8/06 PHYS 34 Modern Phsis Speial relaii I Classial Relaii: Referene Frames Inerial Frame of Referene (IFR): In suh frame, he Newons firs and seond laws of moion appl. Eample: A rain moing a a Consan eloi.

More information

LIGHT and SPECIAL RELATIVITY

LIGHT and SPECIAL RELATIVITY VISUAL PHYSICS ONLINE MODULE 7 NATURE OF LIGHT LIGHT and SPECIAL RELATIVITY LENGTH CONTRACTION RELATIVISTIC ADDITION OF VELOCITIES Time is a relaie quaniy: differen obserers an measuremen differen ime

More information

The Special Theory of Relativity

The Special Theory of Relativity The Speial Theor of Relaii The Speial Theor of Relaii Chaper I. Conradiions in phsis?. Galilean Transformaions of lassial mehanis 3. The effe on Mawell s equaions ligh 4. Mihelson-Morle eperimen 5. insein

More information

Derivation of longitudinal Doppler shift equation between two moving bodies in reference frame at rest

Derivation of longitudinal Doppler shift equation between two moving bodies in reference frame at rest Deriaion o longiudinal Doppler shi equaion beween wo moing bodies in reerene rame a res Masanori Sao Honda Eleronis Co., d., Oyamazuka, Oiwa-ho, Toyohashi, ihi 44-393, Japan E-mail: msao@honda-el.o.jp

More information

Deriving the Useful Expression for Time Dilation in the Presence Of the Gravitation by means of a Light Clock

Deriving the Useful Expression for Time Dilation in the Presence Of the Gravitation by means of a Light Clock IOSR Journal of Applied Physis (IOSR-JAP) e-issn: 78-486Volue 7, Issue Ver II (Mar - Apr 5), PP 7- wwwiosrjournalsorg Deriing he Useful xpression for Tie Dilaion in he Presene Of he Graiaion by eans of

More information

Modern Physics. Two major parts: modern relativity, first 4-6 lectures

Modern Physics. Two major parts: modern relativity, first 4-6 lectures Modern Physis Fall/Winer 900, Max Plank s paper Ueber das Gesez der Energieereilung im Normalsperum, Annalen der Physik IV, 553 (90 peak in 90s/30s Two major pars: modern relaiiy, firs 4-6 leures Quanum

More information

1 st axiom: PRINCIPLE OF RELATIVITY The laws of physics are the same in every inertial frame of reference.

1 st axiom: PRINCIPLE OF RELATIVITY The laws of physics are the same in every inertial frame of reference. SPECIAL ELATIVITY Alber EINSTEIN inrodued his SPECIAL THEOY OF ELATIVITY in 905. To undersand he heory, we will firs reiew he bakground, he heoreial and experimenal deelopmens sine Newon. SPECIAL means

More information

Chapter 12: Velocity, acceleration, and forces

Chapter 12: Velocity, acceleration, and forces To Feel a Force Chaper Spring, Chaper : A. Saes of moion For moion on or near he surface of he earh, i is naural o measure moion wih respec o objecs fixed o he earh. The 4 hr. roaion of he earh has a measurable

More information

Physics 235 Chapter 2. Chapter 2 Newtonian Mechanics Single Particle

Physics 235 Chapter 2. Chapter 2 Newtonian Mechanics Single Particle Chaper 2 Newonian Mechanics Single Paricle In his Chaper we will review wha Newon s laws of mechanics ell us abou he moion of a single paricle. Newon s laws are only valid in suiable reference frames,

More information

Velocity is a relative quantity

Velocity is a relative quantity Veloci is a relaie quani Disenangling Coordinaes PHY2053, Fall 2013, Lecure 6 Newon s Laws 2 PHY2053, Fall 2013, Lecure 6 Newon s Laws 3 R. Field 9/6/2012 Uniersi of Florida PHY 2053 Page 8 Reference Frames

More information

On Einstein s Non-Simultaneity, Length-Contraction and Time-Dilation. Johan F Prins

On Einstein s Non-Simultaneity, Length-Contraction and Time-Dilation. Johan F Prins On Einsein s Non-Simulaneiy, engh-conraion and Time-Dilaion Johan F Prins CATHODIXX, P. O. Bo 537, Cresa 8, Gaueng, Souh Afia Non-simulaneiy of wo simulaneous eens whih our a differen posiions wihin an

More information

A Dynamic Approach to De Broglie's Theory

A Dynamic Approach to De Broglie's Theory Apeiron, Vol., No. 3, Jly 5 74 A Dynami Approah o De Broglie's Theory Nizar Hamdan Deparmen of Physis, Uniersiy of Aleppo P.O. Box 83, Aleppo, SYRIA e-mail:nhamdan59@homail.om Einsein's relaiiy (SRT) [],

More information

Special relativity. The Michelson-Morley experiment

Special relativity. The Michelson-Morley experiment Speial relaiiy Aording o he Twin Parado, a spae raeler leaing his win broher behind on Earh, migh reurn some years laer o find ha his win has aged muh more han he has, or, if he spen a lifeime in spae,

More information

Energy Momentum Tensor for Photonic System

Energy Momentum Tensor for Photonic System 018 IJSST Volume 4 Issue 10 Prin ISSN : 395-6011 Online ISSN : 395-60X Themed Seion: Siene and Tehnology Energy Momenum Tensor for Phooni Sysem ampada Misra Ex-Gues-Teaher, Deparmens of Eleronis, Vidyasagar

More information

A New Formulation of Electrodynamics

A New Formulation of Electrodynamics . Eleromagnei Analysis & Appliaions 1 457-461 doi:1.436/jemaa.1.86 Published Online Augus 1 hp://www.sirp.org/journal/jemaa A New Formulaion of Elerodynamis Arbab I. Arbab 1 Faisal A. Yassein 1 Deparmen

More information

Einstein built his theory of special relativity on two fundamental assumptions or postulates about the way nature behaves.

Einstein built his theory of special relativity on two fundamental assumptions or postulates about the way nature behaves. In he heory of speial relaiviy, an even, suh as he launhing of he spae shule in Figure 8., is a physial happening ha ours a a erain plae and ime. In his drawing wo observers are wahing he lif-off, one

More information

The Full Mathematics of: SPECIAL Relativity. By: PRASANNA PAKKIAM

The Full Mathematics of: SPECIAL Relativity. By: PRASANNA PAKKIAM The Fll Mahemais of: SPECIL Relaii : PRSNN PKKIM CONTENTS INTRODUCTION 3 TIME DILTION & LENGTH CONTRCTION 4 LORENZ TRNSFORMTIONS & COMPOSITION OF VELOCITIES 6 RELTIVISTIC MSS RELTIVISTIC ENERGY 3 ibliograph

More information

The Lorentz Transformation

The Lorentz Transformation The Lorenz Transformaion Relaiviy and Asrophysics Lecure 06 Terry Herer Ouline Coordinae ransformaions Lorenz Transformaion Saemen Proof Addiion of velociies Parial proof Examples of velociy addiion Proof

More information

Lorentz Transformation Properties of Currents for the Particle-Antiparticle Pair Wave Functions

Lorentz Transformation Properties of Currents for the Particle-Antiparticle Pair Wave Functions Open Aess Library Journal 17, Volume 4, e373 ISSN Online: 333-971 ISSN Prin: 333-975 Lorenz Transformaion Properies of Currens for he Parile-Aniparile Pair Wave Funions Raja Roy Deparmen of Eleronis and

More information

MOMENTUM CONSERVATION LAW

MOMENTUM CONSERVATION LAW 1 AAST/AEDT AP PHYSICS B: Impulse and Momenum Le us run an experimen: The ball is moving wih a velociy of V o and a force of F is applied on i for he ime inerval of. As he resul he ball s velociy changes

More information

Equations of motion for constant acceleration

Equations of motion for constant acceleration Lecure 3 Chaper 2 Physics I 01.29.2014 Equaions of moion for consan acceleraion Course websie: hp://faculy.uml.edu/andriy_danylo/teaching/physicsi Lecure Capure: hp://echo360.uml.edu/danylo2013/physics1spring.hml

More information

LAB # 2 - Equilibrium (static)

LAB # 2 - Equilibrium (static) AB # - Equilibrium (saic) Inroducion Isaac Newon's conribuion o physics was o recognize ha despie he seeming compleiy of he Unierse, he moion of is pars is guided by surprisingly simple aws. Newon's inspiraion

More information

Amit Mehra. Indian School of Business, Hyderabad, INDIA Vijay Mookerjee

Amit Mehra. Indian School of Business, Hyderabad, INDIA Vijay Mookerjee RESEARCH ARTICLE HUMAN CAPITAL DEVELOPMENT FOR PROGRAMMERS USING OPEN SOURCE SOFTWARE Ami Mehra Indian Shool of Business, Hyderabad, INDIA {Ami_Mehra@isb.edu} Vijay Mookerjee Shool of Managemen, Uniersiy

More information

Suggested Problem Solutions Associated with Homework #5

Suggested Problem Solutions Associated with Homework #5 Suggesed Problem Soluions Associaed wih Homework #5 431 (a) 8 Si has proons and neurons (b) 85 3 Rb has 3 proons and 48 neurons (c) 5 Tl 81 has 81 proons and neurons 43 IDENTIFY and SET UP: The ex calculaes

More information

Module 2 F c i k c s la l w a s o s f dif di fusi s o i n

Module 2 F c i k c s la l w a s o s f dif di fusi s o i n Module Fick s laws of diffusion Fick s laws of diffusion and hin film soluion Adolf Fick (1855) proposed: d J α d d d J (mole/m s) flu (m /s) diffusion coefficien and (mole/m 3 ) concenraion of ions, aoms

More information

Physics for Scientists and Engineers. Chapter 2 Kinematics in One Dimension

Physics for Scientists and Engineers. Chapter 2 Kinematics in One Dimension Physics for Scieniss and Engineers Chaper Kinemaics in One Dimension Spring, 8 Ho Jung Paik Kinemaics Describes moion while ignoring he agens (forces) ha caused he moion For now, will consider moion in

More information

(Radiation Dominated) Last Update: 21 June 2006

(Radiation Dominated) Last Update: 21 June 2006 Chaper Rik s Cosmology uorial: he ime-emperaure Relaionship in he Early Universe Chaper he ime-emperaure Relaionship in he Early Universe (Radiaion Dominaed) Las Updae: 1 June 006 1. Inroduion n In Chaper

More information

Chapter 2. Motion along a straight line

Chapter 2. Motion along a straight line Chaper Moion along a sraigh line Kinemaics & Dynamics Kinemaics: Descripion of Moion wihou regard o is cause. Dynamics: Sudy of principles ha relae moion o is cause. Basic physical ariables in kinemaics

More information

INSTANTANEOUS VELOCITY

INSTANTANEOUS VELOCITY INSTANTANEOUS VELOCITY I claim ha ha if acceleraion is consan, hen he elociy is a linear funcion of ime and he posiion a quadraic funcion of ime. We wan o inesigae hose claims, and a he same ime, work

More information

A Special Hour with Relativity

A Special Hour with Relativity A Special Hour wih Relaiviy Kenneh Chu The Graduae Colloquium Deparmen of Mahemaics Universiy of Uah Oc 29, 2002 Absrac Wha promped Einsen: Incompaibiliies beween Newonian Mechanics and Maxwell s Elecromagneism.

More information

Unit 1 Test Review Physics Basics, Movement, and Vectors Chapters 1-3

Unit 1 Test Review Physics Basics, Movement, and Vectors Chapters 1-3 A.P. Physics B Uni 1 Tes Reiew Physics Basics, Moemen, and Vecors Chapers 1-3 * In sudying for your es, make sure o sudy his reiew shee along wih your quizzes and homework assignmens. Muliple Choice Reiew:

More information

One-Dimensional Kinematics

One-Dimensional Kinematics One-Dimensional Kinemaics One dimensional kinemaics refers o moion along a sraigh line. Een hough we lie in a 3-dimension world, moion can ofen be absraced o a single dimension. We can also describe moion

More information

Linear Quadratic Regulator (LQR) - State Feedback Design

Linear Quadratic Regulator (LQR) - State Feedback Design Linear Quadrai Regulaor (LQR) - Sae Feedbak Design A sysem is expressed in sae variable form as x = Ax + Bu n m wih x( ) R, u( ) R and he iniial ondiion x() = x A he sabilizaion problem using sae variable

More information

Mass Transfer Coefficients (MTC) and Correlations I

Mass Transfer Coefficients (MTC) and Correlations I Mass Transfer Mass Transfer Coeffiiens (MTC) and Correlaions I 7- Mass Transfer Coeffiiens and Correlaions I Diffusion an be desribed in wo ways:. Deailed physial desripion based on Fik s laws and he diffusion

More information

The Maxwell Equations, the Lorentz Field and the Electromagnetic Nanofield with Regard to the Question of Relativity

The Maxwell Equations, the Lorentz Field and the Electromagnetic Nanofield with Regard to the Question of Relativity The Maxwell Equaions, he Lorenz Field and he Elecromagneic Nanofield wih Regard o he Quesion of Relaiviy Daniele Sasso * Absrac We discuss he Elecromagneic Theory in some main respecs and specifically

More information

Q.1 Define work and its unit?

Q.1 Define work and its unit? CHP # 6 ORK AND ENERGY Q.1 Define work and is uni? A. ORK I can be define as when we applied a force on a body and he body covers a disance in he direcion of force, hen we say ha work is done. I is a scalar

More information

Generalized electromagnetic energy-momentum tensor and scalar curvature of space at the location of charged particle

Generalized electromagnetic energy-momentum tensor and scalar curvature of space at the location of charged particle Generalized eleromagnei energy-momenum ensor and salar urvaure of spae a he loaion of harged parile A.L. Kholmeskii 1, O.V. Missevih and T. Yarman 3 1 Belarus Sae Universiy, Nezavisimosi Avenue, 0030 Minsk,

More information

NEWTON S SECOND LAW OF MOTION

NEWTON S SECOND LAW OF MOTION Course and Secion Dae Names NEWTON S SECOND LAW OF MOTION The acceleraion of an objec is defined as he rae of change of elociy. If he elociy changes by an amoun in a ime, hen he aerage acceleraion during

More information

Analysis of Tubular Linear Permanent Magnet Motor for Drilling Application

Analysis of Tubular Linear Permanent Magnet Motor for Drilling Application Analysis of Tubular Linear Permanen Magne Moor for Drilling Appliaion Shujun Zhang, Lars Norum, Rober Nilssen Deparmen of Eleri Power Engineering Norwegian Universiy of Siene and Tehnology, Trondheim 7491

More information

Linear Response Theory: The connection between QFT and experiments

Linear Response Theory: The connection between QFT and experiments Phys540.nb 39 3 Linear Response Theory: The connecion beween QFT and experimens 3.1. Basic conceps and ideas Q: How do we measure he conduciviy of a meal? A: we firs inroduce a weak elecric field E, and

More information

Chapter 3 Kinematics in Two Dimensions

Chapter 3 Kinematics in Two Dimensions Chaper 3 KINEMATICS IN TWO DIMENSIONS PREVIEW Two-dimensional moion includes objecs which are moing in wo direcions a he same ime, such as a projecile, which has boh horizonal and erical moion. These wo

More information

Phys 221 Fall Chapter 2. Motion in One Dimension. 2014, 2005 A. Dzyubenko Brooks/Cole

Phys 221 Fall Chapter 2. Motion in One Dimension. 2014, 2005 A. Dzyubenko Brooks/Cole Phys 221 Fall 2014 Chaper 2 Moion in One Dimension 2014, 2005 A. Dzyubenko 2004 Brooks/Cole 1 Kinemaics Kinemaics, a par of classical mechanics: Describes moion in erms of space and ime Ignores he agen

More information

Interpretation of special relativity as applied to earth-centered locally inertial

Interpretation of special relativity as applied to earth-centered locally inertial Inerpreaion of special relaiviy as applied o earh-cenered locally inerial coordinae sysems in lobal osiioning Sysem saellie experimens Masanori Sao Honda Elecronics Co., Ld., Oyamazuka, Oiwa-cho, Toyohashi,

More information

Notes follow and parts taken from sources in Bibliography

Notes follow and parts taken from sources in Bibliography PHYS 33 Noes follow and pars aken from soures in ibliograph leromoie Fore To begin suding elerodnamis, we firs look a he onneion beween fields and urrens. We an wrie Ohm s law, whih ou hae seen in inroduor

More information

A New Formulation of Quantum Mechanics

A New Formulation of Quantum Mechanics Journal of Modern Physis 3 63-69 hp://dxdoiorg/436/jmp3 Published Online February (hp://wwwsirporg/journal/jmp) A New Formulaion of Quanum Mehanis A I Arbab Faisal A Yassein Deparmen of Physis Fauly of

More information

Number of modes per unit volume of the cavity per unit frequency interval is given by: Mode Density, N

Number of modes per unit volume of the cavity per unit frequency interval is given by: Mode Density, N SMES404 - LASER PHYSCS (LECTURE 5 on /07/07) Number of modes per uni volume of he aviy per uni frequeny inerval is given by: 8 Mode Densiy, N (.) Therefore, energy densiy (per uni freq. inerval); U 8h

More information

Molecular Motion in Isotropic Turbulence

Molecular Motion in Isotropic Turbulence Moleular Moion in Isoropi Turbulene Jing Fan, Jian-Zheng Jiang, and Fei Fei Laboraory of High Temperaure Gas Dynamis, Insiue of Mehanis Chinese Aademy of Sienes, Being 9, China Absra Moleular moion in

More information

Problem Set 9 Due December, 7

Problem Set 9 Due December, 7 EE226: Random Proesses in Sysems Leurer: Jean C. Walrand Problem Se 9 Due Deember, 7 Fall 6 GSI: Assane Gueye his problem se essenially reviews Convergene and Renewal proesses. No all exerises are o be

More information

SPH3U: Projectiles. Recorder: Manager: Speaker:

SPH3U: Projectiles. Recorder: Manager: Speaker: SPH3U: Projeciles Now i s ime o use our new skills o analyze he moion of a golf ball ha was ossed hrough he air. Le s find ou wha is special abou he moion of a projecile. Recorder: Manager: Speaker: 0

More information

Ground Rules. PC1221 Fundamentals of Physics I. Kinematics. Position. Lectures 3 and 4 Motion in One Dimension. A/Prof Tay Seng Chuan

Ground Rules. PC1221 Fundamentals of Physics I. Kinematics. Position. Lectures 3 and 4 Motion in One Dimension. A/Prof Tay Seng Chuan Ground Rules PC11 Fundamenals of Physics I Lecures 3 and 4 Moion in One Dimension A/Prof Tay Seng Chuan 1 Swich off your handphone and pager Swich off your lapop compuer and keep i No alking while lecure

More information

( ) is the stretch factor, and x the

( ) is the stretch factor, and x the (Lecures 7-8) Liddle, Chaper 5 Simple cosmological models (i) Hubble s Law revisied Self-similar srech of he universe All universe models have his characerisic v r ; v = Hr since only his conserves homogeneiy

More information

Integration of the equation of motion with respect to time rather than displacement leads to the equations of impulse and momentum.

Integration of the equation of motion with respect to time rather than displacement leads to the equations of impulse and momentum. Inegraion of he equaion of moion wih respec o ime raher han displacemen leads o he equaions of impulse and momenum. These equaions greal faciliae he soluion of man problems in which he applied forces ac

More information

We may write the basic equation of motion for the particle, as

We may write the basic equation of motion for the particle, as We ma wrie he basic equaion of moion for he paricle, as or F m dg F F linear impulse G dg G G G G change in linear F momenum dg The produc of force and ime is defined as he linear impulse of he force,

More information

The Paradox of Twins Described in a Three-dimensional Space-time Frame

The Paradox of Twins Described in a Three-dimensional Space-time Frame The Paradox of Twins Described in a Three-dimensional Space-ime Frame Tower Chen E_mail: chen@uguam.uog.edu Division of Mahemaical Sciences Universiy of Guam, USA Zeon Chen E_mail: zeon_chen@yahoo.com

More information

Two Coupled Oscillators / Normal Modes

Two Coupled Oscillators / Normal Modes Lecure 3 Phys 3750 Two Coupled Oscillaors / Normal Modes Overview and Moivaion: Today we ake a small, bu significan, sep owards wave moion. We will no ye observe waves, bu his sep is imporan in is own

More information

2.3 SCHRÖDINGER AND HEISENBERG REPRESENTATIONS

2.3 SCHRÖDINGER AND HEISENBERG REPRESENTATIONS Andrei Tokmakoff, MIT Deparmen of Chemisry, 2/22/2007 2-17 2.3 SCHRÖDINGER AND HEISENBERG REPRESENTATIONS The mahemaical formulaion of he dynamics of a quanum sysem is no unique. So far we have described

More information

Week 1 Lecture 2 Problems 2, 5. What if something oscillates with no obvious spring? What is ω? (problem set problem)

Week 1 Lecture 2 Problems 2, 5. What if something oscillates with no obvious spring? What is ω? (problem set problem) Week 1 Lecure Problems, 5 Wha if somehing oscillaes wih no obvious spring? Wha is ω? (problem se problem) Sar wih Try and ge o SHM form E. Full beer can in lake, oscillaing F = m & = ge rearrange: F =

More information

IB Physics Kinematics Worksheet

IB Physics Kinematics Worksheet IB Physics Kinemaics Workshee Wrie full soluions and noes for muliple choice answers. Do no use a calculaor for muliple choice answers. 1. Which of he following is a correc definiion of average acceleraion?

More information

3.1.3 INTRODUCTION TO DYNAMIC OPTIMIZATION: DISCRETE TIME PROBLEMS. A. The Hamiltonian and First-Order Conditions in a Finite Time Horizon

3.1.3 INTRODUCTION TO DYNAMIC OPTIMIZATION: DISCRETE TIME PROBLEMS. A. The Hamiltonian and First-Order Conditions in a Finite Time Horizon 3..3 INRODUCION O DYNAMIC OPIMIZAION: DISCREE IME PROBLEMS A. he Hamilonian and Firs-Order Condiions in a Finie ime Horizon Define a new funcion, he Hamilonian funcion, H. H he change in he oal value of

More information

Chapter 15: Phenomena. Chapter 15 Chemical Kinetics. Reaction Rates. Reaction Rates R P. Reaction Rates. Rate Laws

Chapter 15: Phenomena. Chapter 15 Chemical Kinetics. Reaction Rates. Reaction Rates R P. Reaction Rates. Rate Laws Chaper 5: Phenomena Phenomena: The reacion (aq) + B(aq) C(aq) was sudied a wo differen emperaures (98 K and 35 K). For each emperaure he reacion was sared by puing differen concenraions of he 3 species

More information

1. The graph below shows the variation with time t of the acceleration a of an object from t = 0 to t = T. a

1. The graph below shows the variation with time t of the acceleration a of an object from t = 0 to t = T. a Kinemaics Paper 1 1. The graph below shows he ariaion wih ime of he acceleraion a of an objec from = o = T. a T The shaded area under he graph represens change in A. displacemen. B. elociy. C. momenum.

More information

Let us start with a two dimensional case. We consider a vector ( x,

Let us start with a two dimensional case. We consider a vector ( x, Roaion marices We consider now roaion marices in wo and hree dimensions. We sar wih wo dimensions since wo dimensions are easier han hree o undersand, and one dimension is a lile oo simple. However, our

More information

Physics for Scientists and Engineers I

Physics for Scientists and Engineers I Physics for Scieniss and Engineers I PHY 48, Secion 4 Dr. Beariz Roldán Cuenya Universiy of Cenral Florida, Physics Deparmen, Orlando, FL Chaper - Inroducion I. General II. Inernaional Sysem of Unis III.

More information

B Signals and Systems I Solutions to Midterm Test 2. xt ()

B Signals and Systems I Solutions to Midterm Test 2. xt () 34-33B Signals and Sysems I Soluions o Miderm es 34-33B Signals and Sysems I Soluions o Miderm es ednesday Marh 7, 7:PM-9:PM Examiner: Prof. Benoi Boule Deparmen of Elerial and Compuer Engineering MGill

More information

EE40 Summer 2005: Lecture 2 Instructor: Octavian Florescu 1. Measuring Voltages and Currents

EE40 Summer 2005: Lecture 2 Instructor: Octavian Florescu 1. Measuring Voltages and Currents Announemens HW # Due oday a 6pm. HW # posed online oday and due nex Tuesday a 6pm. Due o sheduling onflis wih some sudens, lasses will resume normally his week and nex. Miderm enaively 7/. EE4 Summer 5:

More information

where the coordinate X (t) describes the system motion. X has its origin at the system static equilibrium position (SEP).

where the coordinate X (t) describes the system motion. X has its origin at the system static equilibrium position (SEP). Appendix A: Conservaion of Mechanical Energy = Conservaion of Linear Momenum Consider he moion of a nd order mechanical sysem comprised of he fundamenal mechanical elemens: ineria or mass (M), siffness

More information

Lecture 2-1 Kinematics in One Dimension Displacement, Velocity and Acceleration Everything in the world is moving. Nothing stays still.

Lecture 2-1 Kinematics in One Dimension Displacement, Velocity and Acceleration Everything in the world is moving. Nothing stays still. Lecure - Kinemaics in One Dimension Displacemen, Velociy and Acceleraion Everyhing in he world is moving. Nohing says sill. Moion occurs a all scales of he universe, saring from he moion of elecrons in

More information

ESCI 343 Atmospheric Dynamics II Lesson 8 Sound Waves

ESCI 343 Atmospheric Dynamics II Lesson 8 Sound Waves ESCI 343 Amoheri Dynami II Leon 8 Sond Wae Referene: An Inrodion o Dynami Meeorology (3 rd ediion), JR Holon Wae in Flid, J Lighhill SOUND WAVES We will limi or analyi o ond wae raeling only along he -ai,

More information

Physics Notes - Ch. 2 Motion in One Dimension

Physics Notes - Ch. 2 Motion in One Dimension Physics Noes - Ch. Moion in One Dimension I. The naure o physical quaniies: scalars and ecors A. Scalar quaniy ha describes only magniude (how much), NOT including direcion; e. mass, emperaure, ime, olume,

More information

Homework Solution Set # 3. Thursday, September 22, Textbook: Claude Cohen Tannoudji, Bernard Diu and Franck Lalo, Second Volume Complement G X

Homework Solution Set # 3. Thursday, September 22, Textbook: Claude Cohen Tannoudji, Bernard Diu and Franck Lalo, Second Volume Complement G X Deparmen of Physics Quanum Mechanics II, 570 Temple Universiy Insrucor: Z.-E. Meziani Homework Soluion Se # 3 Thursday, Sepember, 06 Texbook: Claude Cohen Tannoudji, Bernard Diu and Franck Lalo, Second

More information

Twin Paradox Revisited

Twin Paradox Revisited Twin Parado Revisied Relaiviy and Asrophysics Lecure 19 Terry Herer Ouline Simulaneiy Again Sample Problem L- Twin Parado Revisied Time dilaion viewpoin Lengh conracion viewpoin Parado & why i s no! Problem

More information

CHAPTER 15 SPECIAL RELATIVITY

CHAPTER 15 SPECIAL RELATIVITY CHAPTER 5 SPECIAL RELATIVITY 5 Inroduion Why a haper on relaiviy in a book on lassial mehanis? A firs euse migh be ha he phrase lassial mehanis is used by differen auhors o mean differen hings To some,

More information

Chapter 10 INDUCTANCE Recommended Problems:

Chapter 10 INDUCTANCE Recommended Problems: Chaper 0 NDUCTANCE Recommended Problems: 3,5,7,9,5,6,7,8,9,,,3,6,7,9,3,35,47,48,5,5,69, 7,7. Self nducance Consider he circui shown in he Figure. When he swich is closed, he curren, and so he magneic field,

More information

MEI Mechanics 1 General motion. Section 1: Using calculus

MEI Mechanics 1 General motion. Section 1: Using calculus Soluions o Exercise MEI Mechanics General moion Secion : Using calculus. s 4 v a 6 4 4 When =, v 4 a 6 4 6. (i) When = 0, s = -, so he iniial displacemen = - m. s v 4 When = 0, v = so he iniial velociy

More information

(1) (2) Differentiation of (1) and then substitution of (3) leads to. Therefore, we will simply consider the second-order linear system given by (4)

(1) (2) Differentiation of (1) and then substitution of (3) leads to. Therefore, we will simply consider the second-order linear system given by (4) Phase Plane Analysis of Linear Sysems Adaped from Applied Nonlinear Conrol by Sloine and Li The general form of a linear second-order sysem is a c b d From and b bc d a Differeniaion of and hen subsiuion

More information

Basic solution to Heat Diffusion In general, one-dimensional heat diffusion in a material is defined by the linear, parabolic PDE

Basic solution to Heat Diffusion In general, one-dimensional heat diffusion in a material is defined by the linear, parabolic PDE New Meio e yd 5 ydrology Program Quaniaie Meods in ydrology Basi soluion o ea iffusion In general one-dimensional ea diffusion in a maerial is defined by e linear paraboli PE or were we assume a is defined

More information

Proposal of atomic clock in motion: Time in moving clock

Proposal of atomic clock in motion: Time in moving clock Proposal of aomic clock in moion: Time in moving clock Masanori Sao Honda Elecronics Co., d., 0 Oyamazuka, Oiwa-cho, Toyohashi, ichi 441-3193, Japan E-mail: msao@honda-el.co.jp bsrac: The ime in an aomic

More information

CHEAPEST PMT ONLINE TEST SERIES AIIMS/NEET TOPPER PREPARE QUESTIONS

CHEAPEST PMT ONLINE TEST SERIES AIIMS/NEET TOPPER PREPARE QUESTIONS CHEAPEST PMT ONLINE TEST SERIES AIIMS/NEET TOPPER PREPARE QUESTIONS For more deails see las page or conac @aimaiims.in Physics Mock Tes Paper AIIMS/NEET 07 Physics 06 Saurday Augus 0 Uni es : Moion in

More information

I. OBJECTIVE OF THE EXPERIMENT.

I. OBJECTIVE OF THE EXPERIMENT. I. OBJECTIVE OF THE EXPERIMENT. Swissmero raels a high speeds hrough a unnel a low pressure. I will hereore undergo ricion ha can be due o: ) Viscosiy o gas (c. "Viscosiy o gas" eperimen) ) The air in

More information

Structural Dynamics and Earthquake Engineering

Structural Dynamics and Earthquake Engineering Srucural Dynamics and Earhquae Engineering Course 1 Inroducion. Single degree of freedom sysems: Equaions of moion, problem saemen, soluion mehods. Course noes are available for download a hp://www.c.up.ro/users/aurelsraan/

More information

Matlab and Python programming: how to get started

Matlab and Python programming: how to get started Malab and Pyhon programming: how o ge sared Equipping readers he skills o wrie programs o explore complex sysems and discover ineresing paerns from big daa is one of he main goals of his book. In his chaper,

More information

Laplace transfom: t-translation rule , Haynes Miller and Jeremy Orloff

Laplace transfom: t-translation rule , Haynes Miller and Jeremy Orloff Laplace ransfom: -ranslaion rule 8.03, Haynes Miller and Jeremy Orloff Inroducory example Consider he sysem ẋ + 3x = f(, where f is he inpu and x he response. We know is uni impulse response is 0 for

More information

6.003 Homework #9 Solutions

6.003 Homework #9 Solutions 6.003 Homework #9 Soluions Problems. Fourier varieies a. Deermine he Fourier series coefficiens of he following signal, which is periodic in 0. x () 0 3 0 a 0 5 a k a k 0 πk j3 e 0 e j πk 0 jπk πk e 0

More information

CHAPTER 12 DIRECT CURRENT CIRCUITS

CHAPTER 12 DIRECT CURRENT CIRCUITS CHAPTER 12 DIRECT CURRENT CIUITS DIRECT CURRENT CIUITS 257 12.1 RESISTORS IN SERIES AND IN PARALLEL When wo resisors are conneced ogeher as shown in Figure 12.1 we said ha hey are conneced in series. As

More information

Kinematics in two dimensions

Kinematics in two dimensions Lecure 5 Phsics I 9.18.13 Kinemaics in wo dimensions Course websie: hp://facul.uml.edu/andri_danlo/teaching/phsicsi Lecure Capure: hp://echo36.uml.edu/danlo13/phsics1fall.hml 95.141, Fall 13, Lecure 5

More information

Diffusion & Viscosity: Navier-Stokes Equation

Diffusion & Viscosity: Navier-Stokes Equation 4/5/018 Diffusion & Viscosiy: Navier-Sokes Equaion 1 4/5/018 Diffusion Equaion Imagine a quaniy C(x,) represening a local propery in a fluid, eg. - hermal energy densiy - concenraion of a polluan - densiy

More information

Millennium Theory of Relativity

Millennium Theory of Relativity Millennium Theory of Relaiiy Copyrigh 001 Joseph A. Rybzyk Absra The Millennium Theory of Relaiiy is a funamenal heory in relaiisi physis. Through mehoial analysis of he eiene, srong an onining argumens

More information

) were both constant and we brought them from under the integral.

) were both constant and we brought them from under the integral. YIELD-PER-RECRUIT (coninued The yield-per-recrui model applies o a cohor, bu we saw in he Age Disribuions lecure ha he properies of a cohor do no apply in general o a collecion of cohors, which is wha

More information

PHYSICS 149: Lecture 9

PHYSICS 149: Lecture 9 PHYSICS 149: Lecure 9 Chaper 3 3.2 Velociy and Acceleraion 3.3 Newon s Second Law of Moion 3.4 Applying Newon s Second Law 3.5 Relaive Velociy Lecure 9 Purdue Universiy, Physics 149 1 Velociy (m/s) The

More information

KINEMATICS IN ONE DIMENSION

KINEMATICS IN ONE DIMENSION KINEMATICS IN ONE DIMENSION PREVIEW Kinemaics is he sudy of how hings move how far (disance and displacemen), how fas (speed and velociy), and how fas ha how fas changes (acceleraion). We say ha an objec

More information