Physics 43 HW 2 Chapter 39 Problems given from 7 th Edition
|
|
- Melvin Fisher
- 5 years ago
- Views:
Transcription
1 Physis 3 HW Chater 39 Problems gien from 7 th Edition Problems:, 7,, 9, 1, 0,,, 9, 33, 35, 3, 0, 5,. How fast must a meter stik be moing if its length is measured to shrink to m? P39. L = L L Taking L = where L = 1.00 m gies L = L L 1 = = = 0.66 L 7. An atomi lok moes at km/h for 1.00 h as measured by an idential lok on the Earth. How many nanoseonds slow will the moing lok be omared with the Earth lok, at the end of the 1.00 h interal? P39.7 Δ t = γδ t = Δt so Δ t = Δt 1 t Δ and If then Δ t Δ t = Δt 1.00 = km h = = 77. m s s = 9.6 and Δt Δ t = s = 1.5 s = 1.5 ns 7. A muon formed high in the Earth s atmoshere traels at seed = for a distane of.60 km before it deays into an eletron, a neutrino, and an antineutrino ( μ + + ) e. (a) How long does the muon lie, as measured in its referene frame? How far does the muon trael, as measured in its frame? P39. For =, γ = (a) The muon s lifetime as measured in the Earth s rest frame is.60 km Δ t = and the lifetime measured in the muon s rest frame is 3 Δ t 1.60 Δ t = = = γ ( 3.00 s).1 μs 3 L.60 L = L = = = 69 m γ 7.09
2 9. A saeraft with a roer length of 300 m takes μs to ass an Earth obserer. Determine the seed of the saeraft as measured by the Earth obserer. P39.9 The saeshi is measured by the Earth obserer to be length-ontrated to oerhead by: L = L or L = L Also, the ontrated length is related to the time required to ass L = t or L = t = ( t) Equating these two exressions gies L L = ( t) or + = L t L Using the gien alues: L = 300 m and 7 t = 7.50 s this beomes giing = = The idential twins Seedo and Goslo join a migration from the Earth to Planet X. It is 0.0 ly away in a referene frame in whih both lanets are at rest. The twins, of the same age, deart at the same time on different saeraft. Seedo s raft traels steadily at 0.950, and Goslo s at Calulate the age differene between the twins after Goslo s saeraft lands on Planet X. Whih twin is the older? P39.1 In the Earth frame, Seedo s tri lasts for a time Δx 0.0 ly Δ t = = = 1.05 yr ly yr Seedo s age adanes only by the roer time interal Δt Δ t = = 1.05 yr 0.95 = 6.57 yr during his tri γ Similarly for Goslo, Δx 0.0 ly Δ t = = 0.75 = 17.6 yr ly yr While Seedo has landed on Planet X and is waiting for his brother, he ages by 0.0 ly 0.0 ly = 5.61 yr ly yr ly yr Then Goslo ends u older by 17.6 yr ( 6.57 yr yr ) = 5.5 yr.
3 0. A moing rod is obsered to hae a length of.00 m and to be oriented at an angle of 30.0 with reset to the diretion of motion, as shown in Figure P39.3. The rod has a seed of (a) What is the roer length of the rod? What is the orientation angle in the roer frame? 1 1 P39.0 γ = = = We are also gien: L 1 =.00 m, and θ = 30.0 (both measured in a referene frame moing relatie to the rod). L = L osθ =.00 m 0.67 = 1.73 m x Thus, 1x 1 1 and L = L sin θ = (.00 m )( 0.500) = 1.00 m 1y 1 1 L is a roer length, related to by x L1x L1x = L γ Therefore, L =.0L = 17.3 m x 1x and L = L1 = 1.00 m (Lengths erendiular to the motion are unhanged). (a) L ( L ) ( L ) = + gies L = 17. m x y y y L 1 y θ = tan gies θ = 3.30 L x A red light flashes at osition xr = 3.00 m and time tr = s, and a blue light flashes at xb B = 5.00 m and tbb = s, all measured in the S referene frame. Referene frame S has its origin at the same oint as S at t = t = 0; frame S moes uniformly to the right. Both flashes are obsered to our at the same lae in S. (a) Find the relatie seed between S and S. Find the loation of the two flashes in frame S. () At what time does the red flash our in the S frame? P39. (a) From the Lorentz transformation, the searations between the blue-light and red-light eents are desribed by Δ x = γ ( Δx Δ t) 0 = γ.00 m (.00 s).00 m = =.50 s.00 s 1 γ = = s 3.00 s Again from the Lorentz transformation, x = γ ( x t) : x = m (.50 s)( 1.00 s) x =.97 m () t = γ t x : (.50 s) ( 3.00 s) t = s ( 3.00 m ) t = 1.33 s
4 . A Klingon saeraft moes away from the Earth at a seed of 0.00 (Fig. P39.6). The starshi Enterrise ursues at a seed of relatie to the Earth. Obserers on the Earth see the Enterrise oertaking the Klingon raft at a relatie seed of 0.0. With what seed is the Enterrise oertaking the Klingon raft as seen by the rew of the Enterrise? P39. u x = Enterrise eloity = Klingon eloity From Equation ux u x = = = u x An unstable artile at rest breaks into two fragments of unequal mass. The mass of the first fragment is.50 kg, and that of the other is kg. If the lighter fragment has a seed of 0.93 after the breaku, what is the seed of the heaier fragment? P39.9 Relatiisti momentum of the system of fragments must be onsered. For total momentum to be zero after as it was before, we must hae, with subsrit referring to the heaier fragment, and subsrit 1 to the lighter, = 1 or or.50 kg γmu = γ1mu 1 1 = ( 1.67 kg) ( u ) Proeeding to sole, we find u (.960 kg) = u = and u = ( 0.93 ) 7 u u 1 = 33. Find the momentum of a roton in MeV/ units assuming its total energy is twie its rest energy. P39.33 E= γ m = m or γ = Thus, u 1 3 = = or γ 3 u = The momentum is then 3 m = γ mu = m = M ev 3 M ev = 3 = 1.63
5 35. A roton moes at Calulate its (a) rest energy, total energy, and () kineti energy. P39.35 (a) E m R 7 = = 1.67 kg.99 s = 1.50 J= 93 M ev 1.50 J 1 E= γ m = =.1 J = 3.00 M ev ( 0.950) 3 () 3 K = E m =.1 J 1.50 J= 3.31 J=.07 M ev 3. In a tyial olor teleision iture tube, the eletrons are aelerated through a otential differene of V. (a) What seed do the eletrons hae when they strike the sreen? What is their kineti energy in joules? P39.3 (a) ( Δ ) = = ( γ ) 1 e q V K m 1 q ΔV ev Thus, γ = = 1+ = 1+ = 1.09 u m e ev so 1 (u/) = and u= K ( γ ) me q( V) = 1 = Δ = 1.60 C.50 J C =.00 J Consider eletrons aelerated to an energy of 0.0 GeV in the 3.00 km long Stanford Linear Aelerator. (a) What is the γ fator for the eletrons? What is their seed? () How long does the aelerator aear to them? P39.0 (a) E= γ m = 0.0 GeV with m = M ev for eletrons. 0.0 ev Thus, γ = = ev γ = = 3.91 from whih u= u () 3 u L 3.00 L = L = = = 7.67 = γ m 5. The ower outut of the Sun is W. How muh mass is onerted to energy in the Sun eah seond? P39.5 de dm dm dt dt dt 6 P = = = = 3.5 W Thus, dm dt J s 9 = =. kg s ( 3.00 s)
6
Relativity. Chapter 26. Quick Quizzes
Chater 6 elatiity Quik Quizzes. (a). Less time will hae assed for you in your frame of referene than for your emloyer bak on Earth. Thus, to maximize your ayhek, you should hoose to hae your ay alulated
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 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 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 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 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 informationRelativity III. Review: Kinetic Energy. Example: He beam from THIA K = 300keV v =? Exact vs non-relativistic calculations Q.37-3.
Relatiity III Today: Time dilation eamples The Lorentz Transformation Four-dimensional spaetime The inariant interal Eamples Reiew: Kineti Energy General relation for total energy: Rest energy, 0: Kineti
More informationIf the speed of light were smaller than it is, would relativistic phenomena be more or less conspicuous than they are now?
Physis 07 Problem. If the speed of light were smaller than it is, would relatiisti phenomena be more or less onspiuous than they are now? All of the phenomena of speial relatiity depend upon the fator
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 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 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 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 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 informationfiziks Institute for NET/JRF, GATE, IIT JAM, JEST, TIFR and GRE in PHYSICAL SCIENCES CLASSICAL MECHANICS SOLUTIONS
fizis CLASSICAL MECHANICS SOLUTIONS GATE- Q. For the set of all Lorentz transforations with eloities along the x-axis onsider the two stateents gien below: P: If L is a Lorentz transforation then, L -
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 informationAnnouncements. Today s class. The Lorentz transformation. Lorentz transformation (Relativistic version of Galileo transformation)
Announements Reading for Monda:. -.5 HW 3 is posted. Due net Wed. noon. The Frida was a TYPO! IT I DUE WEDNEDAY! Toda s lass Lorent transformation Doppler shift First Midterm is on the 6 th. Will oer relatiit
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 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 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 information8.022 (E&M) Lecture 11
8.0 (E&M) Leture Topis: Introdution to Speial Relatiit Length ontration and Time dilation Lorentz transformations Veloit transformation Speial relatiit Read for the hallenge? Speial relatiit seems eas
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 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 informationChapter 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 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 informationTime Contraction: The Possibility of Faster Than Light without Violation of Lorentz Transformation or Causality and the Vacuum Energy Dependent
Artile International Journal of Modern Theoretial Physis, 014, 3(1): 44-73 International Journal of Modern Theoretial Physis Journal homepage:www.modernsientifipress.om/journals/ijmtp.aspx ISSN: 169-746
More informationTest of General Relativity Theory by Investigating the Conservation of Energy in a Relativistic Free Fall in the Uniform Gravitational Field
Test of General Relatiity Theory by Inestigating the Conseration of Energy in a Relatiisti Free Fall in the Uniform Graitational Field By Jarosla Hyneek 1 Abstrat: This paper inestigates the General Relatiity
More informationPHYSICS FOR THE IB DIPLOMA CAMBRIDGE UNIVERSITY PRESS
Option A Relatiity A The beginnings of relatiity Learning objeties It is said that Albert Einstein, as a boy, asked himself what would happen if he held a mirror in front of himself and ran forward at
More informationRelativity and Astrophysics Lecture 10 Terry Herter. Doppler Shift The Expanding Universe Hubble s discovery
Doppler Eet Doppler Eet Relatiity and Astrophysis Leture 0 Terry Herter Outline Doppler Shit The Expanding Unierse Hubble s disoery Reading Spaetime Physis: Chapter 4 Problem L-, page (due today/monday)
More informationRelativistic Analysis of Doppler Effect and Aberration based on Vectorial Lorentz Transformations
Uniersidad Central de Venezuela From the SeletedWorks of Jorge A Frano June, Relatiisti Analysis of Doppler Effet and Aberration based on Vetorial Lorentz Transformations Jorge A Frano, Uniersidad Central
More informationJournal of Physical Mathematics
Journal of Physial Mathematis Researh Artile Artile Journal of Physial Mathematis Makanae, J Phys Math 207, 8: DOI: 0.472/2090-0902.00025 OMICS Open International Aess Verifying Einstein s Time by Using
More informationAnnouncements. Review: Lorentz & velocity transformations (relativistic version of Galileo) Transformations (in 1D) Some examples
Announeents Reading for Monda: Chapter.6-. First Mid-ter is in das (Feb. 9 th, 7:30p). It will oer Chapters &. Reiew: Lorentz & eloit transforations (relatiisti ersion of Galileo) Transforations (in D)
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 informationThe Thomas Precession Factor in Spin-Orbit Interaction
p. The Thomas Preession Fator in Spin-Orbit Interation Herbert Kroemer * Department of Eletrial and Computer Engineering, Uniersity of California, Santa Barbara, CA 9306 The origin of the Thomas fator
More informationJournal of Theoretics Vol.5-2 Guest Commentary Relativistic Thermodynamics for the Introductory Physics Course
Journal of heoretis Vol.5- Guest Commentary Relatiisti hermodynamis for the Introdutory Physis Course B.Rothenstein bernhard_rothenstein@yahoo.om I.Zaharie Physis Department, "Politehnia" Uniersity imisoara,
More informationVolume Charge Density in Most General Lorentz Transformation
Publiations Aailable Online J. Si. Res. 8(), 59-65 (016) JOURNA OF SCIENTIFIC RESEARCH www.banglajol.info/inde.php/jsr Volume Charge Densit in Most General orent Transformation S. A. Bhuian *, A. R. Baiid
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 information, an inverse square law.
Uniform irular motion Speed onstant, but eloity hanging. and a / t point to enter. s r θ > θ s/r t / r, also θ in small limit > t/r > a / r, entripetal aeleration Sine a points to enter of irle, F m a
More informationτ = 10 seconds . In a non-relativistic N 1 = N The muon survival is given by the law of radioactive decay N(t)=N exp /.
Muons on the moon Time ilation using ot prouts Time ilation using Lorentz boosts Cheking the etor formula Relatiisti aition of eloities Why you an t eee the spee of light by suessie boosts Doppler shifts
More informationHigh Energy Astrophysics
High Energ Astrophsis Essentials Giampaolo Pisano Jodrell Bank Centre for Astrophsis - Uniersit of Manhester giampaolo.pisano@manhester.a.uk - http://www.jb.man.a.uk/~gp/ Februar 01 Essentials - Eletromagneti
More informationAgenda 2/12/2017. Modern Physics for Frommies V Gravitation Lecture 6. Special Relativity Einstein s Postulates. Einstein s Postulates
/1/17 Fromm Institute for Lifelong Learning Uniersit of San Franiso Modern Phsis for Frommies V Graitation Leture 6 Agenda Speial Relatiit Einstein s Postulates 15 Februar 17 Modern Phsis V Leture 6 1
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 informationMoment of inertia: (1.3) Kinetic energy of rotation: Angular momentum of a solid object rotating around a fixed axis: Wave particle relationships: ω =
FW Phys 13 E:\Exel files\h 18 Reiew of FormulasM3.do page 1 of 6 Rotational formulas: (1.1) The angular momentum L of a point mass m, moing with eloity is gien by the etor produt between its radius etor
More informationDoppler-Voigt-Einstein Selforganization The Mechanism for Information Transfer
Apeiron, Vol. 7, No., Otober Doppler-Voigt-Einstein Selforganization The ehanism for Information Transfer Jiří Stáek Laboratory of Diffusion Proesses Prague, Czeh Republi Email: staek@olny.z Doppler-Voigt-Einstein
More informationSPH4U UNIVERSITY PHYSICS
SPH4U UNIVERSITY PHYSICS REVOLUTIONS IN MODERN PHYSICS:... L (P.588-591) Special Relatiity Time dilation is only one of the consequences of Einstein s special theory of relatiity. Since reference frames
More informationPhysicsAndMathsTutor.com 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
More informationLinear Momentum and Collisions Conservation of linear momentum
Unit 4 Linear omentum and Collisions 4.. Conseration of linear momentum 4. Collisions 4.3 Impulse 4.4 Coefficient of restitution (e) 4.. Conseration of linear momentum m m u u m = u = u m Before Collision
More informationTransformation of Orbital Angular Momentum and Spin Angular Momentum
Aerian Jornal of Matheatis and Statistis 6, 65: 3-6 DOI: 593/jajs6653 Transforation of Orbital Anglar Moent and Spin Anglar Moent Md Tarek Hossain *, Md Shah Ala Departent of Physis, Shahjalal Uniersity
More informationSpecial Relativity Electromagnetic and Gravitation combined Into one theory
--5 Speial Relatiity Eletromagneti and Graitation ombined Into one theory Mourii Shahter mourii@gmail.om mourii@walla.o.il ISRAE, HOON 54-54855 Introdution In this paper, I try to ombine Eletromagneti
More informationMOTION OF AN ELECTRON IN CLASSICAL AND RELATIVISTIC ELECTRODYNAMICS AND AN ALTERNATIVE ELECTRODYNAMICS
1 MOTION OF AN ELECTRON IN CLASSICAL AND RELATIVISTIC ELECTRODYNAMICS AND AN ALTERNATIVE ELECTRODYNAMICS Musa D. Abdullahi 1 Bujumbura Street, Wuse, Abuja, Nigeria E-mail: musadab@outlook.om Abstrat As
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 informationOn the quantitative effects
International Journal of Modern Physis and Appliation 4; (): 8-4 Published online September, 4 (http://www.aasit.org/journal/ijmpa) On the quantitatie effets Chang-Wei Hu Beijing Relatiity Theory Researh
More informationSpecial Relativity. Overview. Historical Background. Reading. Chris Prior. Trinity College Oxford. and
Overview Seial Relativit Chris Prior ASTeC RAL Trinit College Oford and The rinile of seial relativit Lorentz transformation and onsequenes Sae-time 4-vetors: osition, veloit, momentum, invariants, ovariane.
More informationSpecial relativity. Announcements:
Announcements: Special relatiity Homework solutions are posted! Remember problem soling sessions on Tuesday from 1-3pm in G140. Homework is due on Wednesday at 1:00pm in wood cabinet in G2B90 Hendrik Lorentz
More informationPseudo-Superluminal Motion 1
seudo-superluminal Motion 1 On seudo-superluminal Motion Anamitra alit Author /Teaher(free-laner physiist),india,154 Motijheel Aenue,Kolkata:700074 palit.anamitra@gmail.om h:91-33-5514464 Abstrat: Modern
More informationElectromagnetic Theory Prof. Ruiz, UNC Asheville, doctorphys on YouTube Chapter B Notes. Special Relativity. B1. The Rotation Matrix
Eletromagneti Theory Prof. Ruiz, UNC Asheille, dotorphys on YouTube Chapter B Notes. Speial Relatiity B1. The Rotation Matrix There are two pairs of axes below. The prime axes are rotated with respet to
More informationSpecial Relativity Simply Debunked in Five Steps!
Speial Relatiity Simply Debunked in Fie Steps! Radwan M. Kassir Abstrat The speed of light postulate is losely examined from the perspetie of two inertial referene frames unprimed ( stationary ) and primed
More informationOn the Logical Inconsistency of the Special Theory of Relativity. Stephen J. Crothers. 22 nd February, 2017
To ite this paper: Amerian Journal of Modern Physis. Vol. 6 No. 3 07 pp. 43-48. doi: 0.648/j.ajmp.070603. On the Logial Inonsisteny of the Speial Theory of Relatiity Stephen J. Crothers thenarmis@yahoo.om
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 informationPhysics Courseware Modern Physics
Physis Cousewae oden Physis Enegy and oentu Relatiisti oentu: p γ Kineti enegy: K. E. ( γ ) Auxiliay equation: E + 4 p whee is the est ass and E is total enegy. Poble.- What has oe ass at est: i) A sodiu
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 informationEspen Gaarder Haug Norwegian University of Life Sciences January 5, 2017
Einstein ersus FitzGerald, Lorentz, and Larmor Length Contration Einstein s Length Contration is Also Consistent with Anisotropi One-Way Speed of Light Espen Gaarder Haug Norwegian Uniersity of Life Sienes
More informationVII. Relativistic optics. Electromagnetic fields in inertial frames of reference. dt j ( ) ψ = 0. ri r j. Galilean transformation
VII. Relatiisti optis eletromagneti fields in inertial frames of referene VII. Relatiisti optis Eletromagneti fields in inertial frames of referene Galilean transformation Before 1900 the spae and time
More informationIntroduction to Relativistic Mechanics and the Concept of Mass
Introdution to Relatiisti Mehanis and the Conept of Mass Gron Tudor Jones Uniersity of Birmingham CRN HST014 Introdution to relatiisti kinematis and the onept of mass Mass is one of the most fundamental
More informationGeneral Physics I. Lecture 20: Lorentz Transformation. Prof. WAN, Xin ( 万歆 )
General Physics I Lecture 20: Lorentz Transformation Prof. WAN, Xin ( 万歆 ) xinwan@zju.edu.cn http://zimp.zju.edu.cn/~xinwan/ Outline Lorentz transformation The inariant interal Minkowski diagram; Geometrical
More informationElectromagnetism and Relativity
Chapter 6: Idea 5 Eletromagnetism and Relatiity The fats are relatie, but the law is absolute. When you understand this statement, then you understand Relatiity! Introdution We hae taken an historial approah
More informationPhysics 2D Lecture Slides Lecture : Jan 11th 200. First Quiz This Friday!
Physis D Letre Slides Letre : Jan 11th 00 Viek Sharma UCSD Physis First Qiz This Friday! Bring a Ble Book, allator; hek battery Make sre yo remember the ode nmber for this ose gien to yo (reord it some
More informationSpecial relativity. x' = x vt y' = y z' = z t' = t Galilean transformation. = dx' dt. = dx. u' = dx' dt'
PHYS-3 Relatiity. Notes for Physics and Higher Physics b. Joe Wolfe See also our web pages: http://www.phys.unsw.edu.au/~jw/time.html http://www.phys.unsw.edu.au/~jw/relatiity.html http://www.phys.unsw.edu.au/~jw/twin.html
More informationSPECTRUM OF THE COMA CLUSTER RADIO HALO SYNCHROTRON RADIATION
SPECTRUM OF THE COMA CLUSTER RADIO HALO SYNCHROTRON RADIATION OUTLINE OF THE LESSON REMINDER SPECIAL RELATIVITY: BEAMING, RELATIVISTIC LARMOR FORMULA CYCLOTRON EMISSION SYNCHROTRON POWER AND SPECTRUM EMITTED
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 informationPhysics 4A Solutions to Chapter 4 Homework
Physics 4A Solutions to Chapter 4 Homework Chapter 4 Questions: 4, 1, 1 Exercises & Problems: 5, 11, 3, 7, 8, 58, 67, 77, 87, 11 Answers to Questions: Q 4-4 (a) all tie (b) 1 and tie (the rocket is shot
More informationCh. 38: Special Relativity End of Chapter Problem Solutions
Ch 3: Speial Relativity End of Chapter Problem Solutions 1 Chasing Light In order to arry out the onversions in this exerise, we use the standard method of multiplying by unity You do not hange the value
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 informationPhysics 2D Lecture Slides Lecture 7: Jan 14th 2004
Quiz is This Friday Quiz will over Setions.-.6 (inlusive) Remaining material will be arried over to Quiz Bring Blue Book, hek alulator battery Write all answers in indelible ink else no grade! Write answers
More informationRed Shift and Blue Shift: A realistic approach
Red Shift and Blue Shift: A ealisti appoah Benhad Rothenstein Politehnia Uniesity of Timisoaa, Physis Dept., Timisoaa, Romania E-mail: benhad_othenstein@yahoo.om Coina Nafonita Politehnia Uniesity of Timisoaa,
More informationPhysics Essays volume 16, number 3, 2003
Physis Essays olume 6, number 3, 003 Calulation of So-Called General Relatiisti Phenomena by Adaning Newton s Theory of Graitation, Maintaining Classial Coneptions of Spae and Relatiity Reiner Georg Ziefle
More informationGeneral Physics I. Lecture 18: Lorentz Transformation. Prof. WAN, Xin ( 万歆 )
General Physics I Lecture 18: Lorentz Transformation Prof. WAN, Xin ( 万歆 ) xinwan@zju.edu.cn http://zimp.zju.edu.cn/~xinwan/ Outline Experimental erification of the special theory Lorentz transformation
More informationChapter 4 Two-Dimensional Kinematics. Copyright 2010 Pearson Education, Inc.
Chapter 4 Two-Dimensional Kinematics Units of Chapter 4 Motion in Two Dimensions Projectile Motion: Basic Equations Zero Launch Angle General Launch Angle Projectile Motion: Key Characteristics 4-1 Motion
More informationWould you risk your live driving drunk? Intro
Martha Casquete Would you risk your lie driing drunk? Intro Motion Position and displacement Aerage elocity and aerage speed Instantaneous elocity and speed Acceleration Constant acceleration: A special
More informationTAP 702-6: Binary stars
TAP 702-6: Binary stars Orbiting binary stars: A type of ariable star. This type of ariable star onsists of two stars orbiting around eah other. When the dier star is in front of the brighter one, the
More informationMotion in Two and Three Dimensions
PH 1-1D Spring 013 Motion in Two and Three Dimensions Lectures 5,6,7 Chapter 4 (Halliday/Resnick/Walker, Fundamentals of Physics 9 th edition) 1 Chapter 4 Motion in Two and Three Dimensions In this chapter
More informationOn the derivation of the Lorentz-transformation
On the deriation of the Lorentz-transformation Johan F Prins CATHODIXX 8 Portland Plae, Northliff ext. 15, Johannesburg 195, South Afria johanprins@athodixx.om Abstrat The onentional way to derie the equations
More informationMomentum and Energy. Relativity and Astrophysics Lecture 24 Terry Herter. Energy and Momentum Conservation of energy and momentum
Momentum and Energy Relatiity and Astrohysics Lecture 4 Terry Herter Outline Newtonian Physics Energy and Momentum Conseration of energy and momentum Reading Sacetime Physics: Chater 7 Homework: (due Wed.
More informationPHYS 2020 Spring 2012 Announcements
PHYS 2020 Spring 2012 Announements Continuing to adjust the shedule to relet the progress o the letures: HW #7 is now due Mon. Apr 9 1 Chapter 24 Eletromagneti Waes Next 3 hapters on the behaior o light
More informationChapter 26. Relativity
Chapter 26 Relativity Time Dilation The vehicle is moving to the right with speed v A mirror is fixed to the ceiling of the vehicle An observer, O, at rest in this system holds a laser a distance d below
More informationStellar Aberration, Relative Motion, and the Lorentz Factor
ong Beah 010 PROCEEDINGS of the NP 1 Stellar berration, Relatie Motion, and the orentz Fator Joseph. Rybzyk 139 Stetson Drie, Chalfont, P 18914-3751 e-mail: jarybzyk@erizon.net Presented are the results
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 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 informationIntro to Nuclear and Particle Physics (5110)
Intro to Nulear and Partile Physis (5110) Marh 7, 009 Relativisti Kinematis 3/7/009 1 Relativisti Kinematis Review! Wherever you studied this before, look at it again, e.g. Tipler (Modern Physis), Hyperphysis
More informationFOCUS ON CONCEPTS Section 7.1 The Impulse Momentum Theorem
WEEK-6 Recitation PHYS 3 FOCUS ON CONCEPTS Section 7. The Impulse Momentum Theorem Mar, 08. Two identical cars are traeling at the same speed. One is heading due east and the other due north, as the drawing
More informationTHE ESSENTIAL RELATIONSHIP BETWEEN MASS AND ENERGY
Sientifi Inquiry, ol. 8, no., 7, pp. 56 6 IIGSS Aademi Publisher TH SSNTIAL RLATIONSHIP BTWN MASS AND NRGY LI ZIFNG Petroleum ngineering Institute, Yanshan Uniersity, Qinhuangdao, Hebei, 664, China -mail:
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 informationChapter 36 Relativistic Mechanics
Chapter 36 Relatiistic Mechanics What is relatiit? Terminolog and phsical framework Galilean relatiit Einstein s relatiit Eents and measurements imultaneit Time dilation Length contraction Lorentz transformations
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 informationMotion in Two and Three Dimensions
PH 1-A Fall 014 Motion in Two and Three Dimensions Lectures 4,5 Chapter 4 (Halliday/Resnick/Walker, Fundamentals of Physics 9 th edition) 1 Chapter 4 Motion in Two and Three Dimensions In this chapter
More informationl. For adjacent fringes, m dsin m
Test 3 Pratie Problems Ch 4 Wave Nature of Light ) Double Slit A parallel beam of light from a He-Ne laser, with a wavelength of 656 nm, falls on two very narrow slits that are 0.050 mm apart. How far
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 informationSpecial Theory of Relativity
Speial Theory of Relatiity Introdtion: Galileo was first persaded (oaed) that earth is in otion arond the sn, whih is stationary. Most of his fellows (onteporaries) arged that if it is tre then why birds
More informationChapter 26 Special Theory of Relativity
Chapter 26 Special Theory of Relativity Classical Physics: At the end of the 19 th century, classical physics was well established. It seems that the natural world was very well explained. Newtonian mechanics
More informationEinstein's Energy Formula Must Be Revised
Eintein' Energy Formula Mut Be Reied Le Van Cuong uong_le_an@yahoo.om Information from a iene journal how that the dilation of time in Eintein peial relatie theory wa proen by the experiment of ientit
More informationJournal of Theoretics Vol.4-4
Journal of Theoretis ol.4-4 Cherenko s Partiles as Magnetons Dipl. Ing. Andrija Radoić Nike Strugara 3a, 3 Beograd, Yugoslaia Eail: andrijar@eunet.yu Abstrat: The artile will show that the forula for Cherenko
More information