PhysicsAndMathsTutor.com 1
|
|
- Patience Rodgers
- 6 years ago
- Views:
Transcription
1 PhysisAndMathsTutor.om. (a (i beam splitter [or semi-silvered mirror] (ii a ompensator [or a glass blok] allows for the thikness of the (semi-silvered mirror to obtain equal optial path lengths in the two branhes of the apparatus 3 (b (i onentri rings an interferene pattern [alt: whole view shows one shade beause there is a onstant phase differene] (ii fringes [or rings] shift 5 extra for l gives one omplete fringe shift [or fration of wavelength extra auses notieable fringe shift or notieable hange of intensity (if uniform] 4 ( (i rotate apparatus through 9 observe the fringes at the same time observed fringes did not hange [or shift] (ii speed of light in free spae is invariant [or does not depend on motion of soure or observer or no evidene for absolute motion] max 3 []. (a (i l = (t =. 5 9 =.5m (ii l l (..5 = l (3. l. 5 =.59 m
2 PhysisAndMathsTutor.om (b (i m = m or m (. (3. m m =.6m (. (3. [or = or.77 7 kg] kineti energy = (m m [or =.6m or (3 ] = 9. (J (ii total k.e. = ( 7 9. = 9. 5 (J 5 9. k.e. per seond 9 = 6W max 5 5 [] 3. (a no hange in the fringe pattern on rotation the speed of light is the same in the two diretions the speed of light from a light soure on Earth is unaffeted by the motion of the Earth [or the speed of light is invariant or independent of the motion of the soure or observer] the laws of dynamis annot be applied to light no ether max 3 (b (i distane 6Toneyear time = yr speed. (ii L = 6 [or 6 light years] L L = 6(. (=.6 6= 9.6
3 PhysisAndMathsTutor.om 3 (iii t = years t =t = (. =.6 = yr age = + = 33 yr 6 [9] 4. (a (i speed of light (in free spae independent of motion of soure and of motion of observer [alternative (i speed of light is same in all frames of referene ] (ii laws of physis have same form in all inertial frames inertial frame is one in whih Newton s st law of motion obeyed laws of physis unhanged in oordinate transformation from one inertial frame of referene to any other inertial frame max 4 (b (i m m =. 7 kg =. ( (.996 (ii t =. 6 s t t =. 6 (.996 (s =.46 5 (s s(= t = = 736 m
4 PhysisAndMathsTutor.om 4 [alternative (ii 6 l t = 657 (m orret substitution of l in l = l l 657 l =.996 l = 736 m 6 [] 5. (a as speed, mass infinite gain of E k auses large gain of mass when speed is lose to gain of E k auses small gain of speed when speed is lose to E k = ½mv valid at speeds << max 3 QWC (b (i E k = ev =.6 9. (= 3.3(6 9 J (ii (use of m = E k gives gain of mass = 3.7 (kg (3 3.7 = m 7 = m.67 mass of proton = m +m (=3 m 6 9 (using E k = gives gain of mass = 3. 6 (kg 3 m mass of proton = 4 m 4 ( 3 = v v 3 /.99 v =.999 =.99(7 m s 3 [] 6. (a (i (use of v = d gives v = 4 t 6.4 =.(6 m s (ii atual length = 4 m
5 PhysisAndMathsTutor.om 5 (use of v l l / gives /.6 length in partile frame, l = 4 3 (allow C.E. for value of v l = (4.3 = 7(.5 m 4 (b time between two events depends on speed of observer / [or v t t or roket time depends on speed of traveller] traveller s journey time is the proper time between start and stop [or t is the proper time or t is the time on Earth] journey time measured on Earth > journey time measured by traveller [or t > t or roket time slower/less than Earth time] traveller younger than twin on return to Earth 4 [] (i v =.96 m s 5 9 (ii t = 5 ns v t 5 / /.96 = 5 3. = 5 ns QWC [4]
6 PhysisAndMathsTutor.om 6. (a (i two beams (or rays reah the observer interferene takes plae between the two beams bright fringe formed if/where (optial path differene = whole number of wavelengths (or two beams in phase [or dark fringe formed if/where (optial path differene = whole number +.5 wavelengths] (or two beams out of phase by C/ / /½ yle (ii rotation by 9 realigns beams relative to diretion of Earth s motion no shift means no hange in optial path differene between the two beams ( time taken by light to travel to eah mirror unhanged by rotation distane to mirrors is unhanged by rotation ( no shift means that the speed of light is unaffeted [or disproves other theory] max 5 (b the speed of light does not depend on the motion of the light soure or that of the observer [7] 9. (a Newton s laws obeyed in an inertial frame [or inertial frames move at onstant veloity relative to eah other] suitable example (e.g. objet moving at onstant veloity / (b (i (use of t = t gives t = (ns t = 9 (.995 =. 7 s /
7 PhysisAndMathsTutor.om 7 (ii time taken distane = s speed time taken = half-lives, whih is time to derease to 5% intensity / [alternative sheme: (use of l = l v gives l = (m / (.995 l = =. m time taken. = 3.6 s.995 = half-lives, whih is time to derease to 5% intensity ] 5 [7]. (i E k (= ev (= =. (J (.76 (J (ii (use of E = m gives m =. (3 7 =. m 7.m =. 7 (kg.67 (allow C.E. for value of E k from (i, but not 3rd mark m = m + m (=. m / (iii (use of m = m v gives.m = v / =. =.7 m s 7 / [7]
8 PhysisAndMathsTutor.om. (a (i t = (s (use of t = t v gives t = (.994 =73 s (ii distane (=.994t = =. m (. m (allow C.E. for value of t from (i 4 (b spae twin s travel time = proper time (or t time on Earth, t = t v t> t [or time for traveller slows down ompared with Earth twin] spae twin ages less than Earth twin travelling in non-inertial frame of referene max 3 / [7] v. (a m = m v gives =. =.99 v (=.995 =.9(5 m s 3 v (b m = m m infinity as v [or m inreases as v inreases] E k (= m m infinity as v v = would require infinite E k (or mass whih is (physially impossible Max 3 [6] 3. (i time taken dis tane 34 speed (9 s
9 PhysisAndMathsTutor.om 9 (ii use of t = t ( v / / where t = ns and t is the half-life in the detetors frame of referene 9 9 t 57(.6 s / (.95 time taken for π meson to pass from one detetor to the other = half-lives (approx (in the detetors' frame of referene half-lives orrespond to a redution to 5%, so 75% of the π mesons passing the first detetor do not reah the seond detetor alternatives for first 3 marks in (ii. use of t = t ( v /, where t = ns = 57.6(ns (.95 / journey time in detetor frame (= t = 57.6ns ( half-lives. use of t = t ( v / where t = 9 ns = journey time in detetor frame t =37ns journey time in rest frame = ns ( half-lives [5] 4. (a (i speed of light in free spae independent of motion of soure and of motion of observer (ii laws of physis have the same form in all inertial frames inertial frame is one in whih Newton s st law of motion is obeyed laws of physis unhanged in oordinate transformation from one inertial frame to another max 4
10 PhysisAndMathsTutor.om (b (i m (= m ( v / / =.9 (.995 / (kg =.9 7 kg (ii E (= m =.9 7 (3. =.7 J (iii E K (= E m =.7 (.9 (3. =.5 J 6 []
Chapter 26 Lecture Notes
Chapter 26 Leture Notes Physis 2424 - Strauss Formulas: t = t0 1 v L = L0 1 v m = m0 1 v E = m 0 2 + KE = m 2 KE = m 2 -m 0 2 mv 0 p= mv = 1 v E 2 = p 2 2 + m 2 0 4 v + u u = 2 1 + vu There were two revolutions
More informationName Solutions to Test 1 September 23, 2016
Name Solutions to Test 1 September 3, 016 This test onsists of three parts. Please note that in parts II and III, you an skip one question of those offered. Possibly useful formulas: F qequb x xvt E Evpx
More informationSpecial Relativity. Relativity
10/17/01 Speial Relativity Leture 17 Relativity There is no absolute motion. Everything is relative. Suppose two people are alone in spae and traveling towards one another As measured by the Doppler shift!
More information( x vt) m (0.80)(3 10 m/s)( s) 1200 m m/s m/s m s 330 s c. 3.
Solutions to HW 10 Problems and Exerises: 37.. Visualize: At t t t 0 s, the origins of the S, S, and S referene frames oinide. Solve: We have 1 ( v/ ) 1 (0.0) 1.667. (a) Using the Lorentz transformations,
More informationThe Special Theory of Relativity
The Speial Theory of Relatiity Galilean Newtonian Relatiity Galileo Galilei Isaa Newton Definition of an inertial referene frame: One in whih Newton s first law is alid. onstant if F0 Earth is rotating
More informationChapter 35. Special Theory of Relativity (1905)
Chapter 35 Speial Theory of Relatiity (1905) 1. Postulates of the Speial Theory of Relatiity: A. The laws of physis are the same in all oordinate systems either at rest or moing at onstant eloity with
More informationCHAPTER 26 The Special Theory of Relativity
CHAPTER 6 The Speial Theory of Relativity Units Galilean-Newtonian Relativity Postulates of the Speial Theory of Relativity Simultaneity Time Dilation and the Twin Paradox Length Contration Four-Dimensional
More informationRelativistic Dynamics
Chapter 7 Relativisti Dynamis 7.1 General Priniples of Dynamis 7.2 Relativisti Ation As stated in Setion A.2, all of dynamis is derived from the priniple of least ation. Thus it is our hore to find a suitable
More informationChapter Outline The Relativity of Time and Time Dilation The Relativistic Addition of Velocities Relativistic Energy and E= mc 2
Chapter 9 Relativeity Chapter Outline 9-1 The Postulate t of Speial Relativity it 9- The Relativity of Time and Time Dilation 9-3 The Relativity of Length and Length Contration 9-4 The Relativisti Addition
More informationCritical Reflections on the Hafele and Keating Experiment
Critial Refletions on the Hafele and Keating Experiment W.Nawrot In 1971 Hafele and Keating performed their famous experiment whih onfirmed the time dilation predited by SRT by use of marosopi loks. As
More informationDO PHYSICS ONLINE. SPECIAL RELATIVITY Frames of Reference
DO PHYSICS ONLINE SPACE SPECIAL RELATIVITY Frames of Referene Spae travel Apollo 11 spaeraft: Earth Moon v ~ 40x10 3 km.h -1 Voyager spaeraft: v ~ 60x10 3 km.h -1 (no sling shot effet) Ulysses spaeraft:
More informationDepartment of Natural Sciences Clayton State University. Physics 3650 Quiz 1. c. Both kinetic and elastic potential energies can be negative.
Department of Natural Sienes Physis 3650 Quiz 1 August 5, 008 1. Whih one of the statements below is orret? a. Elasti potential energy an be negative but the kineti energy annot. b. Kineti energy an be
More informationRecapitulate. Prof. Shiva Prasad, Department of Physics, IIT Bombay
18 1 Reapitulate We disussed how light an be thought of onsisting of partiles known as photons. Compton Effet demonstrated that they an be treated as a partile with zero rest mass having nonzero energy
More informationRelativity in Classical Physics
Relativity in Classial Physis Main Points Introdution Galilean (Newtonian) Relativity Relativity & Eletromagnetism Mihelson-Morley Experiment Introdution The theory of relativity deals with the study of
More informationThe gravitational phenomena without the curved spacetime
The gravitational phenomena without the urved spaetime Mirosław J. Kubiak Abstrat: In this paper was presented a desription of the gravitational phenomena in the new medium, different than the urved spaetime,
More informationChapter 39 Relativity
Chapter 39 Relatiity from relatie motion to relatiity 39. The Priniple of Galilean Relatiity The laws of mehanis mst be the same in all inertial frames of referene. Galilean spae-time transformation eqations
More informationThe Lorenz Transform
The Lorenz Transform Flameno Chuk Keyser Part I The Einstein/Bergmann deriation of the Lorentz Transform I follow the deriation of the Lorentz Transform, following Peter S Bergmann in Introdution to the
More informationMillennium Relativity Acceleration Composition. The Relativistic Relationship between Acceleration and Uniform Motion
Millennium Relativity Aeleration Composition he Relativisti Relationship between Aeleration and niform Motion Copyright 003 Joseph A. Rybzyk Abstrat he relativisti priniples developed throughout the six
More informationThe Laws of Acceleration
The Laws of Aeleration The Relationships between Time, Veloity, and Rate of Aeleration Copyright 2001 Joseph A. Rybzyk Abstrat Presented is a theory in fundamental theoretial physis that establishes the
More informationRelativity fundamentals explained well (I hope) Walter F. Smith, Haverford College
Relativity fundamentals explained well (I hope) Walter F. Smith, Haverford College 3-14-06 1 Propagation of waves through a medium As you ll reall from last semester, when the speed of sound is measured
More informationThe Concept of Mass as Interfering Photons, and the Originating Mechanism of Gravitation D.T. Froedge
The Conept of Mass as Interfering Photons, and the Originating Mehanism of Gravitation D.T. Froedge V04 Formerly Auburn University Phys-dtfroedge@glasgow-ky.om Abstrat For most purposes in physis the onept
More informationPY Modern Physics
PY 351 - Modern Physis Assignment 6 - Otober 19, 2017. Due in lass on Otober 26, 2017. Assignment 6: Do all six problems. After a base of 4 points (to make the maximum sore equal to 100), eah orret solution
More informationAnswers to Coursebook questions Chapter J2
Answers to Courseook questions Chapter J 1 a Partiles are produed in ollisions one example out of many is: a ollision of an eletron with a positron in a synhrotron. If we produe a pair of a partile and
More informationTWO WAYS TO DISTINGUISH ONE INERTIAL FRAME FROM ANOTHER
TWO WAYS TO DISTINGUISH ONE INERTIAL FRAME FROM ANOTHER (No general ausality without superluminal veloities) by Dr. Tamas Lajtner Correspondene via web site: www.lajtnemahine.om ABSTRACT...2 1. SPACETIME
More informationTime and Energy, Inertia and Gravity
Time and Energy, Inertia and Gravity The Relationship between Time, Aeleration, and Veloity and its Affet on Energy, and the Relationship between Inertia and Gravity Copyright 00 Joseph A. Rybzyk Abstrat
More informationSimple Considerations on the Cosmological Redshift
Apeiron, Vol. 5, No. 3, July 8 35 Simple Considerations on the Cosmologial Redshift José Franiso Garía Juliá C/ Dr. Maro Mereniano, 65, 5. 465 Valenia (Spain) E-mail: jose.garia@dival.es Generally, the
More information12.1 Events at the same proper distance from some event
Chapter 1 Uniform Aeleration 1.1 Events at the same proper distane from some event Consider the set of events that are at a fixed proper distane from some event. Loating the origin of spae-time at this
More informationTWO WAYS TO DISTINGUISH ONE INERTIAL FRAME FROM ANOTHER
TWO WAYS TO DISTINGUISH ONE INERTIAL FRAME FROM ANOTHER (WHY IS THE SPEED OF LIGHT CONSTANT?) Dr. Tamas Lajtner Correspondene via web site: www.lajtnemahine.om. ABSTRACT... 2 2. SPACETIME CONTINUUM BY
More informationName the object labelled B and explain its purpose.
PhysicsAndMathsTutor.com 1 1. The diagram represents the Michelson-Morley interferometer. surface-silvered mirror M 1 l 1 extended source of monochromatic light B surface-silvered mirror M 2 A l 2 viewing
More informationTHEORETICAL PROBLEM 2 SOLUTION DOPPLER LASER COOLING AND OPTICAL MOLASSES. v 1 c
THEOETICA POBEM SOUTION DOPPE ASE COOING AND OPTICA MOASSES The key to this problem is the Doppler effet (to be preise, the longitudinal Doppler effet): The frequeny of a monohromi beam of light deteted
More informationWave Propagation through Random Media
Chapter 3. Wave Propagation through Random Media 3. Charateristis of Wave Behavior Sound propagation through random media is the entral part of this investigation. This hapter presents a frame of referene
More informationTo investigate the relationship between the work done to accelerate a trolley and the energy stored in the moving trolley.
SP2h.1 Aelerating trolleys Your teaher may wath to see if you an follow instrutions safely take areful measurements. Introdution The work done y a fore is a measure of the energy transferred when a fore
More informationarxiv:gr-qc/ v2 6 Feb 2004
Hubble Red Shift and the Anomalous Aeleration of Pioneer 0 and arxiv:gr-q/0402024v2 6 Feb 2004 Kostadin Trenčevski Faulty of Natural Sienes and Mathematis, P.O.Box 62, 000 Skopje, Maedonia Abstrat It this
More informationAharonov-Bohm effect. Dan Solomon.
Aharonov-Bohm effet. Dan Solomon. In the figure the magneti field is onfined to a solenoid of radius r 0 and is direted in the z- diretion, out of the paper. The solenoid is surrounded by a barrier that
More informationLecture 3 - Lorentz Transformations
Leture - Lorentz Transformations A Puzzle... Example A ruler is positioned perpendiular to a wall. A stik of length L flies by at speed v. It travels in front of the ruler, so that it obsures part of the
More informationFinal Review. A Puzzle... Special Relativity. Direction of the Force. Moving at the Speed of Light
Final Review A Puzzle... Diretion of the Fore A point harge q is loated a fixed height h above an infinite horizontal onduting plane. Another point harge q is loated a height z (with z > h) above the plane.
More informationGravity from the Uncertainty Principle.
Gravity from the Unertainty Priniple. M.E. MCulloh Otober 29, 2013 Abstrat It is shown here that Newton's gravity law an be derived from the unertainty priniple. The idea is that as the distane between
More informationInvestigation of the de Broglie-Einstein velocity equation s. universality in the context of the Davisson-Germer experiment. Yusuf Z.
Investigation of the de Broglie-instein veloity equation s universality in the ontext of the Davisson-Germer experiment Yusuf Z. UMUL Canaya University, letroni and Communiation Dept., Öğretmenler Cad.,
More informationBreakdown of the Special Theory of Relativity as Proven by Synchronization of Clocks
Breakdown of the Speial Theory of Relativity as Proven by Synhronization of Cloks Koshun Suto Koshun_suto19@mbr.nifty.om Abstrat In this paper, a hypothetial preferred frame of referene is presumed, and
More informationToday: Review of SR. Einstein s Postulates of Relativity (Abbreviated versions) Let's start with a few important concepts
Today: eiew of Eam: Tomorrow, 7:30-9:00pm, DUANE GB30 You an bring paper (etter format written on both sides with whateer you think might help you during the eam. But you annot bring the tetbook or leture
More informationPhysical Laws, Absolutes, Relative Absolutes and Relativistic Time Phenomena
Page 1 of 10 Physial Laws, Absolutes, Relative Absolutes and Relativisti Time Phenomena Antonio Ruggeri modexp@iafria.om Sine in the field of knowledge we deal with absolutes, there are absolute laws that
More informationOn the Absolute Meaning of Motion
On the Absolute Meaning of Motion H. Edwards Publiation link: https://doi.org/10.1016/j.rinp.2017.09.053 Keywords: Kinematis; Gravity; Atomi Cloks; Cosmi Mirowave Bakground Abstrat The present manusript
More informationParticle-wave symmetry in Quantum Mechanics And Special Relativity Theory
Partile-wave symmetry in Quantum Mehanis And Speial Relativity Theory Author one: XiaoLin Li,Chongqing,China,hidebrain@hotmail.om Corresponding author: XiaoLin Li, Chongqing,China,hidebrain@hotmail.om
More information1. Which two values of temperature are equivalent to the nearest degree when measured on the Kelvin and on the
. Whih two values of teperature are equivalent to the nearest degree when easured on the Kelvin and on the Celsius sales of teperature? Kelvin sale Celsius sale A. 40 33 B. 273 00 C. 33 40 D. 373 0 2.
More informationarxiv:physics/ Oct 2002
Dedution of Lorentz Transformation from the eistene of absolute rest. Dedution of the speed of light in any frame of referene. Rodrigo de Abreu Centro de Eletrodinâmia e Departamento de Físia do IST Abstrat
More informationINTRO VIDEOS. LESSON 9.5: The Doppler Effect
DEVIL PHYSICS BADDEST CLASS ON CAMPUS IB PHYSICS INTRO VIDEOS Big Bang Theory of the Doppler Effet Doppler Effet LESSON 9.5: The Doppler Effet 1. Essential Idea: The Doppler Effet desribes the phenomenon
More informationSpecial and General Relativity
9/16/009 Speial and General Relativity Inertial referene frame: a referene frame in whih an aeleration is the result of a fore. Examples of Inertial Referene Frames 1. This room. Experiment: Drop a ball.
More informationA special reference frame is the center of mass or zero momentum system frame. It is very useful when discussing high energy particle reactions.
High nergy Partile Physis A seial referene frame is the enter of mass or zero momentum system frame. It is very useful when disussing high energy artile reations. We onsider a ollision between two artiles
More informationEinstein s Three Mistakes in Special Relativity Revealed. Copyright Joseph A. Rybczyk
Einstein s Three Mistakes in Speial Relativity Revealed Copyright Joseph A. Rybzyk Abstrat When the evidene supported priniples of eletromagneti propagation are properly applied, the derived theory is
More informationChapter 28 Special Relativity
Galilean Relatiity Chapter 8 Speial Relatiity A passenger in an airplane throws a ball straight up. It appears to oe in a ertial path. The law of graity and equations of otion under unifor aeleration are
More information22.01 Fall 2015, Problem Set 6 (Normal Version Solutions)
.0 Fall 05, Problem Set 6 (Normal Version Solutions) Due: November, :59PM on Stellar November 4, 05 Complete all the assigned problems, and do make sure to show your intermediate work. Please upload your
More informationPHYS-3301 Lecture 4. Chapter 2. Announcement. Sep. 7, Special Relativity. Course webpage Textbook
Announement Course webage htt://www.hys.ttu.edu/~slee/330/ Textbook PHYS-330 Leture 4 HW (due 9/4 Chater 0, 6, 36, 4, 45, 50, 5, 55, 58 Se. 7, 07 Chater Seial Relativity. Basi Ideas. Consequenes of Einstein
More informationWavetech, LLC. Ultrafast Pulses and GVD. John O Hara Created: Dec. 6, 2013
Ultrafast Pulses and GVD John O Hara Created: De. 6, 3 Introdution This doument overs the basi onepts of group veloity dispersion (GVD) and ultrafast pulse propagation in an optial fiber. Neessarily, it
More informationAstr 5465 Mar. 29, 2018 Galactic Dynamics I: Disks
Galati Dynamis Overview Astr 5465 Mar. 29, 2018 Subjet is omplex but we will hit the highlights Our goal is to develop an appreiation of the subjet whih we an use to interpret observational data See Binney
More informationSpecial Relativity Einstein
Speial Relatiity Einstein - 1905 Published 5 papers in Annalen der Physik Photoeletri effet (led to Nobel Prize in 191) Brownian Motion (proed existene of atoms) Speial Relatiity Speial Relatiity (E=m
More information9 Geophysics and Radio-Astronomy: VLBI VeryLongBaseInterferometry
9 Geophysis and Radio-Astronomy: VLBI VeryLongBaseInterferometry VLBI is an interferometry tehnique used in radio astronomy, in whih two or more signals, oming from the same astronomial objet, are reeived
More informationGreen s function for the wave equation
Green s funtion for the wave equation Non-relativisti ase January 2019 1 The wave equations In the Lorentz Gauge, the wave equations for the potentials are (Notes 1 eqns 43 and 44): 1 2 A 2 2 2 A = µ 0
More informationTENSOR FORM OF SPECIAL RELATIVITY
TENSOR FORM OF SPECIAL RELATIVITY We begin by realling that the fundamental priniple of Speial Relativity is that all physial laws must look the same to all inertial observers. This is easiest done by
More informationThe Gravitational Potential for a Moving Observer, Mercury s Perihelion, Photon Deflection and Time Delay of a Solar Grazing Photon
Albuquerque, NM 0 POCEEDINGS of the NPA 457 The Gravitational Potential for a Moving Observer, Merury s Perihelion, Photon Defletion and Time Delay of a Solar Grazing Photon Curtis E. enshaw Tele-Consultants,
More informationDerivation of Non-Einsteinian Relativistic Equations from Momentum Conservation Law
Asian Journal of Applied Siene and Engineering, Volue, No 1/13 ISSN 35-915X(p); 37-9584(e) Derivation of Non-Einsteinian Relativisti Equations fro Moentu Conservation Law M.O.G. Talukder Varendra University,
More informationAnnouncements. Lecture 5 Chapter. 2 Special Relativity. The Doppler Effect
Announements HW1: Ch.-0, 6, 36, 41, 46, 50, 51, 55, 58, 63, 65 *** Lab start-u meeting with TA yesterday; useful? *** Lab manual is osted on the ourse web *** Physis Colloquium (Today 3:40m anelled ***
More informationProblem 3 : Solution/marking scheme Large Hadron Collider (10 points)
Problem 3 : Solution/marking sheme Large Hadron Collider 10 points) Part A. LHC Aelerator 6 points) A1 0.7 pt) Find the exat expression for the final veloity v of the protons as a funtion of the aelerating
More informationECE-320 Linear Control Systems. Winter 2013, Exam 1. No calculators or computers allowed, you may leave your answers as fractions.
ECE-320 Linear Control Systems Winter 2013, Exam 1 No alulators or omputers allowed, you may leave your answers as frations. All problems are worth 3 points unless noted otherwise. Total /100 1 Problems
More informationAddition of velocities. Taking differentials of the Lorentz transformation, relative velocities may be calculated:
Addition of veloities Taking differentials of the Lorentz transformation, relative veloities may be allated: So that defining veloities as: x dx/dt, y dy/dt, x dx /dt, et. it is easily shown that: With
More informationarxiv: v1 [physics.gen-ph] 5 Jan 2018
The Real Quaternion Relativity Viktor Ariel arxiv:1801.03393v1 [physis.gen-ph] 5 Jan 2018 In this work, we use real quaternions and the basi onept of the final speed of light in an attempt to enhane the
More informationphysics/ Nov 1999
Do Gravitational Fields Have Mass? Or on the Nature of Dark Matter Ernst Karl Kunst As has been shown before (a brief omment will be given in the text) relativisti mass and relativisti time dilation of
More informationArmenian Theory of Special Relativity (Illustrated) Robert Nazaryan 1 and Haik Nazaryan 2
29606 Robert Nazaryan Haik Nazaryan/ Elixir Nulear & Radiation Phys. 78 (205) 29606-2967 Available online at www.elixirpublishers.om (Elixir International Journal) Nulear Radiation Physis Elixir Nulear
More information1. RELATIVISTIC KINEMATICS
1. RELATIVISTIC KINEMATICS The one truth of whih the human mind an be ertain indeed, this is the meaning of onsiousness itself is the reognition of its own existene. That we may be seure in this truth
More informationTowards an Absolute Cosmic Distance Gauge by using Redshift Spectra from Light Fatigue.
Towards an Absolute Cosmi Distane Gauge by using Redshift Spetra from Light Fatigue. Desribed by using the Maxwell Analogy for Gravitation. T. De Mees - thierrydemees @ pandora.be Abstrat Light is an eletromagneti
More informationDIGITAL DISTANCE RELAYING SCHEME FOR PARALLEL TRANSMISSION LINES DURING INTER-CIRCUIT FAULTS
CHAPTER 4 DIGITAL DISTANCE RELAYING SCHEME FOR PARALLEL TRANSMISSION LINES DURING INTER-CIRCUIT FAULTS 4.1 INTRODUCTION Around the world, environmental and ost onsiousness are foring utilities to install
More informationStability Analysis of Orbital Motions around Uniformly Rotating Irregular Asteroids
Stability Analysis of Orbital Motions around Uniformly Rotating Irregular Asteroids By Xiyun HoU, ) Daniel J. SCHEERES, ) Xiaosheng XIN, ) Jinglang FENG, ) Jingshi TANG, ) Lin LIU, ) ) Shool of Astronomy
More informationSimultaneity. CHAPTER 2 Special Theory of Relativity 2. Gedanken (Thought) experiments. The complete Lorentz Transformation. Re-evaluation of Time!
CHAPTER Speial Theory of Relatiity. The Need for Aether. The Mihelson-Morley Eperiment.3 Einstein s Postulates.4 The Lorentz Transformation.5 Time Dilation and Length Contration.6 Addition of Veloities.7
More informationRelativistic Addition of Velocities *
OpenStax-CNX module: m42540 1 Relativisti Addition of Veloities * OpenStax This work is produed by OpenStax-CNX and liensed under the Creative Commons Attribution Liense 3.0 Abstrat Calulate relativisti
More informationTutorial 8: Solutions
Tutorial 8: Solutions 1. * (a) Light from the Sun arrives at the Earth, an average of 1.5 10 11 m away, at the rate 1.4 10 3 Watts/m of area perpendiular to the diretion of the light. Assume that sunlight
More informationAnswers to test yourself questions
Answers to test yoursel questions Topi.1 Osilliations 1 a A n osillation is any motion in whih the displaement o a partile rom a ixed point keeps hanging diretion and there is a periodiity in the motion
More information3 Tidal systems modelling: ASMITA model
3 Tidal systems modelling: ASMITA model 3.1 Introdution For many pratial appliations, simulation and predition of oastal behaviour (morphologial development of shorefae, beahes and dunes) at a ertain level
More information). In accordance with the Lorentz transformations for the space-time coordinates of the same event, the space coordinates become
Relativity and quantum mehanis: Jorgensen 1 revisited 1. Introdution Bernhard Rothenstein, Politehnia University of Timisoara, Physis Department, Timisoara, Romania. brothenstein@gmail.om Abstrat. We first
More informationIntroduction to Quantum Chemistry
Chem. 140B Dr. J.A. Mak Introdution to Quantum Chemistry Without Quantum Mehanis, how would you explain: Periodi trends in properties of the elements Struture of ompounds e.g. Tetrahedral arbon in ethane,
More informationMetric of Universe The Causes of Red Shift.
Metri of Universe The Causes of Red Shift. ELKIN IGOR. ielkin@yande.ru Annotation Poinare and Einstein supposed that it is pratially impossible to determine one-way speed of light, that s why speed of
More informationGeneration of EM waves
Generation of EM waves Susan Lea Spring 015 1 The Green s funtion In Lorentz gauge, we obtained the wave equation: A 4π J 1 The orresponding Green s funtion for the problem satisfies the simpler differential
More informationModule 5: Red Recedes, Blue Approaches. UNC-TFA H.S. Astronomy Collaboration, Copyright 2012
Objetives/Key Points Module 5: Red Reedes, Blue Approahes UNC-TFA H.S. Astronomy Collaboration, Copyright 2012 Students will be able to: 1. math the diretion of motion of a soure (approahing or reeding)
More informationRelativistic effects in earth-orbiting Doppler lidar return signals
3530 J. Opt. So. Am. A/ Vol. 4, No. 11/ November 007 Neil Ashby Relativisti effets in earth-orbiting Doppler lidar return signals Neil Ashby 1,, * 1 Department of Physis, University of Colorado, Boulder,
More informationEinstein s theory of special relativity
Einstein s theory of speial relatiity Announements: First homework assignment is online. You will need to read about time dilation (1.8) to answer problem #3 and for the definition of γ for problem #4.
More informationPhysics (Theory) There are 30 questions in total. Question Nos. 1 to 8 are very short answer type questions and carry one mark each.
Physis (Theory) Tie allowed: 3 hours] [Maxiu arks:7 General Instrutions: (i) ll uestions are opulsory. (ii) (iii) (iii) (iv) (v) There are 3 uestions in total. Question Nos. to 8 are very short answer
More informationAcoustic Waves in a Duct
Aousti Waves in a Dut 1 One-Dimensional Waves The one-dimensional wave approximation is valid when the wavelength λ is muh larger than the diameter of the dut D, λ D. The aousti pressure disturbane p is
More informationa) What is the duration of the trip according to Ginette? b) What is the duration of the trip according to Tony?
Ginette stays on Earth while Tony travels towards a star loated 4.6 lightyears away from Earth. The speed of Tony s ship is 80% of the speed of light. www.how-to-draw-artoons-online.om/artoon-earth.html
More informationExperiment 03: Work and Energy
MASSACHUSETTS INSTITUTE OF TECHNOLOGY Physis Department Physis 8.01 Purpose of the Experiment: Experiment 03: Work and Energy In this experiment you allow a art to roll down an inlined ramp and run into
More informationWhere as discussed previously we interpret solutions to this partial differential equation in the weak sense: b
Consider the pure initial value problem for a homogeneous system of onservation laws with no soure terms in one spae dimension: Where as disussed previously we interpret solutions to this partial differential
More informationDoppler Effect (Text 1.3)
Doppler Effet (et 1.3) Consider a light soure as a soure sending out a tik eery 1/ν and these tiks are traeling forward with speed. tik tik tik tik Doppler Effet (et 1.3) Case 1. Obserer oing transersely.
More informationAn ultrasonic air temperature measurement system with self-correction function for humidity
INSTITUTE OFPHYSICS PUBLISHING Meas. Si. Tehnol. 16 (25) 548 555 MEASUREMENTSCIENCE AND TECHNOLOGY doi:1.188/957-233/16/2/3 An ultrasoni air temperature measurement system with self-orretion funtion for
More informationMOVING OBJECTS OBSERVATION THEORY IN PLACE OF SPECIAL RELATIVITY
Inquiry, ol. 8, no., Deember 007, pp. 4 49 IIGSS Aademi Publisher MOVING OBJECTS OBSERVATION THEORY IN PLACE OF SPECIAL RELATIVITY LI ZIFENG Petroleum Engineering Institute, Yanshan Uniersity, Qinhuangdao,
More informationF = c where ^ı is a unit vector along the ray. The normal component is. Iν cos 2 θ. d dadt. dp normal (θ,φ) = dpcos θ = df ν
INTRODUCTION So far, the only information we have been able to get about the universe beyond the solar system is from the eletromagneti radiation that reahes us (and a few osmi rays). So doing Astrophysis
More informationIf velocity of A relative to ground = velocity of B relative to ground = the velocity of A relative to B =
L Physis MC nswers Year:1989 Question Number: 3,0,,4,6,9,30,31,36,40,4 1989MC (3) If eloity of relatie to ground = and eloity of relatie to ground =, then the eloity of relatie to = X X Y Y Suppose that
More informationCALCULATION OF NONLINEAR TUNE SHIFT USING BEAM POSITION MEASUREMENT RESULTS
International Journal of Modern Physis A Vol. 24, No. 5 (2009) 974 986 World Sientifi Publishing Company CALCULATION OF NONLINEAR TUNE SHIFT USING BEAM POSITION MEASUREMENT RESULTS PAVEL SNOPOK, MARTIN
More informationA EUCLIDEAN ALTERNATIVE TO MINKOWSKI SPACETIME DIAGRAM.
A EUCLIDEAN ALTERNATIVE TO MINKOWSKI SPACETIME DIAGRAM. S. Kanagaraj Eulidean Relativity s.kana.raj@gmail.om (1 August 009) Abstrat By re-interpreting the speial relativity (SR) postulates based on Eulidean
More informationA unified field theory; atomic, gravitational orbitals as anti-photons
(plankmomentum.om) A unified field theory; atomi, gravitational orbitals as anti-photons Malolm Maleod E-mail: malem@plankmomentum.om In this essay I propose an alternate interpretation whereby partiles
More informationPhysics 6C. Special Relativity. Prepared by Vince Zaccone For Campus Learning Assistance Services at UCSB
Physis 6C Speial Relatiity Two Main Ideas The Postulates of Speial Relatiity Light traels at the same speed in all inertial referene frames. Laws of physis yield idential results in all inertial referene
More informationA Spatiotemporal Approach to Passive Sound Source Localization
A Spatiotemporal Approah Passive Sound Soure Loalization Pasi Pertilä, Mikko Parviainen, Teemu Korhonen and Ari Visa Institute of Signal Proessing Tampere University of Tehnology, P.O.Box 553, FIN-330,
More informationClass XII - Physics Electromagnetic Waves Chapter-wise Problems
Class XII - Physis Eletromagneti Waves Chapter-wise Problems Multiple Choie Question :- 8 One requires ev of energy to dissoiate a arbon monoxide moleule into arbon and oxygen atoms The minimum frequeny
More informationPHYSICS 212 FINAL EXAM 21 March 2003
PHYSIS INAL EXAM Marh 00 Eam is losed book, losed notes. Use only the provided formula sheet. Write all work and answers in eam booklets. The baks of pages will not be graded unless you so ruest on the
More information