On the Physical Significance of the Lorentz Transformations in SRT. Department of Physics- University of Aleppo, Aleppo- Syria ABSTRACT
|
|
- Elinor Bates
- 5 years ago
- Views:
Transcription
1 On he Phsal Sgnfane of he Loen Tansfomaons n SRT Na Hamdan Sohel aa Depamen of Phss- Unes of leppo leppo- Sa STRCT One show all fas ha seem o eqe he naane of Mawell's feld eqaons nde Loen ansfomaons [nsen's ela []] an be deed fom assmpons dffeen fom hose sed b nsen. In geneal we sa wh he phsal law eqaons [345] and appl he ela pnple o hem. Wh hs appoah nsen's ela SRT s efomlaed n a smple manne ha has dnamal applaon [6] who sng he Loen ansfomaons LT and s knemaal onadons. Ke Wods: Speal Rela Theo Loen Tansfomaon.
2 . Inodon end of he seenh en Gallo's epemens showed ha moon ms be elae n onas o he aeped ew. These epemens led hm also o sae wha s now alled he pnple of Gallean ela he laws of mehans ae he same fo a bod a es and a bod mong a onsan elo. Newon also deeloped hs laws of moon and hs onep of ela he laws of mehans ms be he same n all neal fames. De o Galleo and Newon he onep of absole spae beame edndan b absole me was eaned. The deelopmen of he eleomagne heo n he nneeenh en demonsaed a poblem wh Newonan ela. I seemed noneable o phsss ha M waes old popagae who a medm he ehe. as a onseqene of Newonan ela an obsee mong hogh he ehe wh elo wold mease he elo of a lgh beam as. The Mhelson - Mole epemen showed ha no ehe absole efeene fame esed fo eleomagne phenomena. Ths esl opened he wa fo a new appoah. nsen s ela [] poslaed ha he speed of lgh s naan n all neal fames whh mahemaall led o a new elaonshp beween spaes and me.e. he Loen ansfomaon LT. To emoe he onadon onenng he smmeal popees of spae-me beween lassal mehans and eleodnams he aleed lassal mehans o make ompable wh LT. nsen s mehod [] n deng LT onaned he naane of lgh speed whh was no nlded n Gallan ansfomaon. He onsdeed he Caesan pons n he fame S o be he same n he fame S podng ha we manan he onsan of lgh speed fo he moemen of hs pon n boh fames. Then a pale wh es mass m was eplaed wh he engneeng pon and SRT seeded n applng he pnple of mass eneg eqalene o he mong pale alhogh hs pnple was eale esed o he eleomagne feld befoe. The SRT poslaes fo aos knemaal effes lke lengh onaon and me dlaon. Seeal qesons ase when eamnng hese knemaal effes [98] and man onadons es [7]. Moeoe SRT and pale dnams ae nompable sne he dnams of a mong pale ae esed o aommodae LT. The nompabl beween SRT and pale dnams ases bease LT and s knemaal effes hae pma oe he phsal law n deng he elas dnamal qanes and n he nepeaon of elas phenomena. Ths nompabl an be negleed n m appoah whh begns wh he followng poslaes phsal laws and he ela pnple [345]. - le-magne felds Tansfomaons; elo ansfomaons and Loen-Tansfomaons. The Mawell s eld qaons n fame S ma be epessed as ρ a ; J ε b ; d In pape [4] o nenon was o dee he elas ansfomaon of he eleomagne feld as well as he elas ansfomaon of he hage and en dens. In he soe-fee ase:
3 a ; ; b d ollowng he same eason sed n [4] we now ge he elas ansfomaon of he eleomagne feld.e.; 3 In addon we ge Loen ansfomaon elaons: : 4 O ppose s now o dee he 3 eo elo who LT n he same manne n [3]. We sa fom he Loen foe q 5 ssme ha a haged pale q moes wh elo n fame S. The - omponen of q. 5 s: q 6a Now b applng he ela pnple o qs. 6a he wll pesee he fom n fame S mong wh elo paallel o he ommon - as as follows: q 6b fom qs.6 we hae a Usng qs.3 n qs.7 we ge b 7 8a To oban anohe elas ansfomaon of elo we assme ha he elo n fame S n he fom: 9a q.9a n fame S has he fom: 9b
4 Sbsng q.8a n q.9b we hae / O On he ohe hand q.8a old be wen as O Now we sa fom q. and assmng he ald of qs. and fo he elo n fame S hen q. ma be wen as O 4 4 Usng q.9a n he las elaon afe eaangemen we hae O 3 Compang boh qs. and 3 we ge: 8b
5 The same esl an be deed fom he eqaons 9 f we assme ha and.e.: I s obos ha o deaon poess dffes fom ha n SRT sne LT was no sed n hs poess. s fo he 3-eo elas elo ansfomaons he wee deed as a esl of mahemaal onsdeaons onl who akng no aon he defnon of elo as a ae of hange of poson wh me. Ths s seems naal sne he elo of a pale s no a pa of s nns popees b a meased qan ha old be edefned Deaon he eleomagne feld enso ν fom Loen oe I was known ha he 3-eo fo he eleomagne feld he sala and eo poenal as follows: o s epesened b 4 q.4 defnes a seond ank enso.e.; ν f one we n 4-dmensonal eos whh s wen n hs oodnae ssem ν ν 5 ν 4 ; as 6 ν I s well known ha SRT has emoed he bae beween mae and eneg b eaed a new bae whh an no be ansended aodng o hs heo. Ths bae sepaaes wha s known as he non-elas fom elas phss doman. The phsal laws appopae fo non-elas phss an no ansend hs bae and hene he fom lassal phss. The phsal laws appopae fo
6 elas phss an oe he doman non-elas phss hogh appomaon; and LT beomes a Gallean ansfomaon. The moe sable mehod s o sa wh he laws of lassal phss and make hem onde o all pale eloes.e. o epand he appopaeness of hese laws o deal wh elas doman. s demonsaed n [3] ha elas epessons wee deed begnnng wh he lassal law.e. q and ela pnple. Cona o wha s ofen lamed n SRT we had all he elas epessons n addon he well known phsal law.e.; d ε d q 7 who sng LT and s knemaal effes. whee q.7 epesens he foh omponen of: dp q ν 8 dτ n he 4-eo fomlaon. nd whee τ s he pope elas me P he 4- eo momenm he 4-eo elo and ν he eleomagne feld enso. In hs wa we old fomlae he SRT sang fom a mehanal base [4].e.; dε 9 d d nsead of esng he fomaon of SRT o eleomagne base alone. In pape [6] we onne hs mehod fo he ase of haged pale q mong wh elo n he fame S sbje o an ele feld and a magne fl dens. and hen qs. 9 has he fom d ε q q d d In he pesen pape we onne hs mehod o ge qs.4 and 6 begnnng wh q.. The Caesan omponens of qs. n fame S ae q d a q d b q d dε q d d Mlplng qs.abb and q.d b hen sbang we hae:
7 q d d d d d ε The Loen foe eqaons q. desbes he moon of a haged pale q nde he aon of an eleomagne feld epesened b he enso ν whee 34 s he oodnae ssem and s he 4-d elo eo and P P s he 4-d momenm eo. hs 4-d noaon q. has he fom: ν τ q d dp 3 Whee enso ν has he same fom as n q.6.e.; ν 4 s one know ha he oaon eo n he 4-eo fomlaon has he fom: ν ν ν 5 whee 4 ;. nd f he fnon has he fom ; hen he omponen 4 old be wen n ems of qs.4 and5 as 6a followng he same appoah we fnd 4 and 34 as: 6b 6
8 s well as he omponen 3 3 and has he fom: 7a 7b 7 s one sees now ha he qs. 6 and 7 has he same eo fom as q.4.e.; o 8 4- Deaon he Tansfomaon Relaons of and he Loen Tansfomaons We an now fnd he elas ansfomaon of fo-eo as fo he Loen ansfomaon elaons he wll be deed as a esl of mahemaal onsdeaons onl. Theefoe b wng qs.6b and 7 n fame S aodng o he ela pnple.e.; On he hand we hae also fom q.3 : and hene: 9a 9b Mlplng boh q.9b b and q.9a hen addng he boh eqaons we ge
9 ompang he las elaon wh q.6b we hen hae 3 a nd now f we mlpl boh q.9a b and q.9b b hen addng boh eqaons we ge ompang he las elaon wh q.7 we hen hae 3b In a smla wa f we ewe he elaons 6 and 7b n fame S aodng o he ela pnple and akng no aon elaons 3 we ge 3a 3b Mlplng he boh q.3b b and q.3a hen addng he boh eqaons we ge ompang he las elaon wh q.6 we hen hae 3 geneal eqemen n SRT ha an phsal heo shold be wen n 4-d fom.e."elasall naan" and hen eded o 3-d fom. In m papes we sa del fom he phsal laws wen ognall n 3-d fom o ge he same esls who sng he mos mpoan hng n 4-d fom.e. he me enso. Conlson Can we now see how gea he msonepon s? f we ake he oneps [lengh onaon me dlaon a elo omponen fo a geomeal pon] whh ae sed solel o sole he poblem of he oodnaon of eens we ma se hem o ped he dnamal popees of a pale. Caefl eamnaons of nsen's agmen n hs pape [] leae no dob ha LT s ndeed ansfomaons ha desbe he oodnaes of a phoon. The eo was n assmng ha hese ansfomaons desbe he oodnaes of a maeal pale. The LT ae aall ansfomaon of he oodnaes of a geomeal pon and he
10 do no hae he powe o make pedons abo phsal qanes mass eneg momenm.. LT b o alenae mehod s smpl a neal ansfomaon onanng no phsal sgnfane [345 and 6]. Refeenes - nsen. 95. On he leodnams of Mong odes. nn. Phs GOLDN S.. Non-Knema of he dlaon of me elaon of nsen fo me-neals. Z. Na fosh 55a a Hamdan N. 3. bandonng he Ideas of Lengh Conaon and me dlaon. Gallean leodnams b Hamdan N. 4. bandonng The Idea of Relas Lengh Conaon n Relas leodnams. Gallean leodnams Hamdan N. On he Inaane of Mawell s eld qaons nde Loen Tansfomaons. o appea n Gallean leodnams. 5- Hamdan N. 5. Newon s Seond Low s a Relas law who nsen s Rela. Gallean leodnams Jl./g.. 6- Hamdan N. 5. Deaon of he Relas Dopple ffe fom he Loen oe. peon Vol No. Jan.. 7- HJR S. and GHOSH. 5. Collapse of SRTI: Deaon of eleodnams eqaons fom he Mawell feld eqaons. Gallean eleodnams Vol. 6 p: JIMNKO O. D On he pemenal poofs of elas lengh onaon and me dlaon. Z. Na fosh 53a SHOZHIX Mahemaal and phsal nsffenes of he Loen ansfomaon. Hadon J. opgh. - WILHLM Phsal poblemas of nsen's ela heoes. Hadon J mals: nhamdan@los.om nhamdan59@homal.om
Backcalculation Analysis of Pavement-layer Moduli Using Pattern Search Algorithms
Bakallaon Analyss of Pavemen-laye Modl Usng Paen Seah Algohms Poje Repo fo ENCE 74 Feqan Lo May 7 005 Bakallaon Analyss of Pavemen-laye Modl Usng Paen Seah Algohms. Inodon. Ovevew of he Poje 3. Objeve
More informationChapter 3: Vectors and Two-Dimensional Motion
Chape 3: Vecos and Two-Dmensonal Moon Vecos: magnude and decon Negae o a eco: eese s decon Mulplng o ddng a eco b a scala Vecos n he same decon (eaed lke numbes) Geneal Veco Addon: Tangle mehod o addon
More informationcalculating electromagnetic
Theoeal mehods fo alulang eleomagne felds fom lghnng dshage ajeev Thoapplll oyal Insue of Tehnology KTH Sweden ajeev.thoapplll@ee.kh.se Oulne Despon of he poblem Thee dffeen mehods fo feld alulaons - Dpole
More informationGravity Field and Electromagnetic Field
Gavy Feld and Eleomane Feld Fne Geomeal Feld Theoy o Mae Moon Pa Two Xao Janha Naal ene Fondaon Reseah Gop, hanha Jaoon Unvesy hanha, P.R.C Absa: Gavy eld heoy and eleomane eld heoy ae well esablshed and
More informationChapter Finite Difference Method for Ordinary Differential Equations
Chape 8.7 Fne Dffeence Mehod fo Odnay Dffeenal Eqaons Afe eadng hs chape, yo shold be able o. Undesand wha he fne dffeence mehod s and how o se o solve poblems. Wha s he fne dffeence mehod? The fne dffeence
More informationThe sound field of moving sources
Nose Engneeng / Aoss -- ong Soes The son el o mong soes ong pon soes The pesse el geneae by pon soe o geneal me an The pess T poson I he soe s onenae a he sngle mong pon, soe may I he soe s I be wen as
More informationL4:4. motion from the accelerometer. to recover the simple flutter. Later, we will work out how. readings L4:3
elave moon L4:1 To appl Newon's laws we need measuemens made fom a 'fed,' neal efeence fame (unacceleaed, non-oang) n man applcaons, measuemens ae made moe smpl fom movng efeence fames We hen need a wa
More information5-1. We apply Newton s second law (specifically, Eq. 5-2). F = ma = ma sin 20.0 = 1.0 kg 2.00 m/s sin 20.0 = 0.684N. ( ) ( )
5-1. We apply Newon s second law (specfcally, Eq. 5-). (a) We fnd he componen of he foce s ( ) ( ) F = ma = ma cos 0.0 = 1.00kg.00m/s cos 0.0 = 1.88N. (b) The y componen of he foce s ( ) ( ) F = ma = ma
More informationCHAPTER 10: LINEAR DISCRIMINATION
HAPER : LINEAR DISRIMINAION Dscmnan-based lassfcaon 3 In classfcaon h K classes ( k ) We defned dsmnan funcon g () = K hen gven an es eample e chose (pedced) s class label as f g () as he mamum among g
More informationESS 265 Spring Quarter 2005 Kinetic Simulations
SS 65 Spng Quae 5 Knec Sulaon Lecue une 9 5 An aple of an lecoagnec Pacle Code A an eaple of a knec ulaon we wll ue a one denonal elecoagnec ulaon code called KMPO deeloped b Yohhau Oua and Hoh Mauoo.
More informationMass-Spring Systems Surface Reconstruction
Mass-Spng Syses Physally-Based Modelng: Mass-Spng Syses M. Ale O. Vasles Mass-Spng Syses Mass-Spng Syses Snake pleenaon: Snake pleenaon: Iage Poessng / Sae Reonson: Iage poessng/ Sae Reonson: Mass-Spng
More information1 Constant Real Rate C 1
Consan Real Rae. Real Rae of Inees Suppose you ae equally happy wh uns of he consumpon good oday o 5 uns of he consumpon good n peod s me. C 5 Tha means you ll be pepaed o gve up uns oday n eun fo 5 uns
More informationL-1. Intertemporal Trade in a Two- Period Model
L-. neempoal Tade n a Two- Peod Model Jaek Hník www.jaom-hnk.wbs.z Wha o Shold Alead now en aon def... s a esl of expos fallng sho of mpos. s a esl of savngs fallng sho of nvesmens. S A B NX G B B M X
More informationField due to a collection of N discrete point charges: r is in the direction from
Physcs 46 Fomula Shee Exam Coulomb s Law qq Felec = k ˆ (Fo example, f F s he elecc foce ha q exes on q, hen ˆ s a un veco n he decon fom q o q.) Elecc Feld elaed o he elecc foce by: Felec = qe (elecc
More informationPHYS 1443 Section 001 Lecture #4
PHYS 1443 Secon 001 Lecure #4 Monda, June 5, 006 Moon n Two Dmensons Moon under consan acceleraon Projecle Moon Mamum ranges and heghs Reerence Frames and relae moon Newon s Laws o Moon Force Newon s Law
More informationLecture 5. Chapter 3. Electromagnetic Theory, Photons, and Light
Lecue 5 Chape 3 lecomagneic Theo, Phoons, and Ligh Gauss s Gauss s Faada s Ampèe- Mawell s + Loen foce: S C ds ds S C F dl dl q Mawell equaions d d qv A q A J ds ds In mae fields ae defined hough ineacion
More informationGo over vector and vector algebra Displacement and position in 2-D Average and instantaneous velocity in 2-D Average and instantaneous acceleration
Mh Csquee Go oe eco nd eco lgeb Dsplcemen nd poson n -D Aege nd nsnneous eloc n -D Aege nd nsnneous cceleon n -D Poecle moon Unfom ccle moon Rele eloc* The componens e he legs of he gh ngle whose hpoenuse
More informationMillennium Theory Equations Original Copyright 2002 Joseph A. Rybczyk Updated Copyright 2003 Joseph A. Rybczyk Updated March 16, 2006
Millennim heoy Eqaions Oiginal Copyigh 00 Joseph A. Rybzyk Updaed Copyigh 003 Joseph A. Rybzyk Updaed Mah 6, 006 Following is a omplee lis o he Millennim heoy o Relaiviy eqaions: Fo easy eeene, all eqaions
More informationChapter Finite Difference Method for Ordinary Differential Equations
Chape 8.7 Finie Diffeence Mehod fo Odinay Diffeenial Eqaions Afe eading his chape, yo shold be able o. Undesand wha he finie diffeence mehod is and how o se i o solve poblems. Wha is he finie diffeence
More informationI-POLYA PROCESS AND APPLICATIONS Leda D. Minkova
The XIII Inenaonal Confeence Appled Sochasc Models and Daa Analyss (ASMDA-009) Jne 30-Jly 3, 009, Vlns, LITHUANIA ISBN 978-9955-8-463-5 L Sakalaskas, C Skadas and E K Zavadskas (Eds): ASMDA-009 Seleced
More informationPendulum Dynamics. = Ft tangential direction (2) radial direction (1)
Pendulum Dynams Consder a smple pendulum wh a massless arm of lengh L and a pon mass, m, a he end of he arm. Assumng ha he fron n he sysem s proporonal o he negave of he angenal veloy, Newon s seond law
More informationRotations.
oons j.lbb@phscs.o.c.uk To s summ Fmes of efeence Invnce une nsfomons oon of wve funcon: -funcons Eule s ngles Emple: e e - - Angul momenum s oon geneo Genec nslons n Noehe s heoem Fmes of efeence Conse
More informationName of the Student:
Engneeng Mahemacs 05 SUBJEC NAME : Pobably & Random Pocess SUBJEC CODE : MA645 MAERIAL NAME : Fomula Maeal MAERIAL CODE : JM08AM007 REGULAION : R03 UPDAED ON : Febuay 05 (Scan he above QR code fo he dec
More informationCourse Outline. 1. MATLAB tutorial 2. Motion of systems that can be idealized as particles
Couse Oulne. MATLAB uoal. Moon of syses ha can be dealzed as pacles Descpon of oon, coodnae syses; Newon s laws; Calculang foces equed o nduce pescbed oon; Deng and solng equaons of oon 3. Conseaon laws
More informationby Lauren DeDieu Advisor: George Chen
b Laren DeDe Advsor: George Chen Are one of he mos powerfl mehods o nmercall solve me dependen paral dfferenal eqaons PDE wh some knd of snglar shock waves & blow-p problems. Fed nmber of mesh pons Moves
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 informationA New Approach to Solve Fully Fuzzy Linear Programming with Trapezoidal Numbers Using Conversion Functions
valale Onlne a hp://jnsaa Vol No n 5 Jonal of Ne eseahes n Maheas Sene and eseah Banh IU Ne ppoah o Solve Flly Fzzy nea Pogang h Tapezodal Nes Usng onveson Fnons SH Nasse * Depaen of Maheaal Senes Unvesy
More informations = rθ Chapter 10: Rotation 10.1: What is physics?
Chape : oaon Angula poson, velocy, acceleaon Consan angula acceleaon Angula and lnea quanes oaonal knec enegy oaonal nea Toque Newon s nd law o oaon Wok and oaonal knec enegy.: Wha s physcs? In pevous
More informationNewtonian 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 informationExponential and Logarithmic Equations and Properties of Logarithms. Properties. Properties. log. Exponential. Logarithmic.
Eponenial and Logaihmic Equaions and Popeies of Logaihms Popeies Eponenial a a s = a +s a /a s = a -s (a ) s = a s a b = (ab) Logaihmic log s = log + logs log/s = log - logs log s = s log log a b = loga
More informationPhysics 442. Electro-Magneto-Dynamics. M. Berrondo. Physics BYU
Physis 44 Eleo-Magneo-Dynamis M. Beondo Physis BYU Paaveos Φ= V + Α Φ= V Α = = + J = + ρ J J ρ = J S = u + em S S = u em S Physis BYU Poenials Genealize E = V o he ime dependen E & B ase Podu of paaveos:
More informationModern Energy Functional for Nuclei and Nuclear Matter. By: Alberto Hinojosa, Texas A&M University REU Cyclotron 2008 Mentor: Dr.
Moden Enegy Funconal fo Nucle and Nuclea Mae By: lbeo noosa Teas &M Unvesy REU Cycloon 008 Meno: D. Shalom Shlomo Oulne. Inoducon.. The many-body poblem and he aee-fock mehod. 3. Skyme neacon. 4. aee-fock
More informationRelative and Circular Motion
Relaie and Cicula Moion a) Relaie moion b) Cenipeal acceleaion Mechanics Lecue 3 Slide 1 Mechanics Lecue 3 Slide 2 Time on Video Pelecue Looks like mosly eeyone hee has iewed enie pelecue GOOD! Thank you
More information4/3/2017. PHY 712 Electrodynamics 9-9:50 AM MWF Olin 103
PHY 7 Eleodnais 9-9:50 AM MWF Olin 0 Plan fo Leue 0: Coninue eading Chap Snhoon adiaion adiaion fo eleon snhoon deies adiaion fo asonoial objes in iula obis 0/05/07 PHY 7 Sping 07 -- Leue 0 0/05/07 PHY
More informationSuppose we have observed values t 1, t 2, t n of a random variable T.
Sppose we have obseved vales, 2, of a adom vaable T. The dsbo of T s ow o belog o a cea ype (e.g., expoeal, omal, ec.) b he veco θ ( θ, θ2, θp ) of ow paamees assocaed wh s ow (whee p s he mbe of ow paamees).
More informationCOMPUTER SCIENCE 349A SAMPLE EXAM QUESTIONS WITH SOLUTIONS PARTS 1, 2
COMPUTE SCIENCE 49A SAMPLE EXAM QUESTIONS WITH SOLUTIONS PATS, PAT.. a Dene he erm ll-ondoned problem. b Gve an eample o a polynomal ha has ll-ondoned zeros.. Consder evaluaon o anh, where e e anh. e e
More informationCOORDINATE SYSTEMS, COORDINATE TRANSFORMS, AND APPLICATIONS
Dola Bagaoo 0 COORDINTE SYSTEMS COORDINTE TRNSFORMS ND PPLICTIONS I. INTRODUCTION Smmet coce of coodnate sstem. In solvng Pscs poblems one cooses a coodnate sstem tat fts te poblem at and.e. a coodnate
More informationAPPLICATION OF A Z-TRANSFORMS METHOD FOR INVESTIGATION OF MARKOV G-NETWORKS
Joa of Aed Mahema ad Comaoa Meha 4 3( 6-73 APPLCATON OF A Z-TRANSFORMS METHOD FOR NVESTGATON OF MARKOV G-NETWORKS Mha Maay Vo Nameo e of Mahema Ceohowa Uey of Tehoogy Cęohowa Poad Fay of Mahema ad Come
More informationSections 3.1 and 3.4 Exponential Functions (Growth and Decay)
Secions 3.1 and 3.4 Eponenial Funcions (Gowh and Decay) Chape 3. Secions 1 and 4 Page 1 of 5 Wha Would You Rahe Have... $1million, o double you money evey day fo 31 days saing wih 1cen? Day Cens Day Cens
More informationM. Choudhury 1. and G. C. Hazarika 2
Jonal of led Fld Means Vol. 6 No.. 77-83 3. alable onlne a.jafmonlne.ne ISSN 735-357 ISSN 735-365. e ffes of Vaable Vsos and emal Cond on MHD Osllao Fee Conee Flo as a Veal Plae n Sl Flo Regme Vaable Son
More informationPhysics 201 Lecture 15
Phscs 0 Lecue 5 l Goals Lecue 5 v Elo consevaon of oenu n D & D v Inouce oenu an Iulse Coens on oenu Consevaon l oe geneal han consevaon of echancal eneg l oenu Consevaon occus n sses wh no ne eenal foces
More informationMATHEMATICAL MODEL OF THE DUMMY NECK INCLUDED IN A FRONTAL IMPACT TESTING SYSTEM
he h Inenaonal onfeene Advaned opose Maeals Enneen OMA 8- Oobe Basov Roana MAHEMAIAL MODEL O HE DUMMY NEK INLUDED IN A RONAL IMPA ESIN SYSEM unel Sefana Popa Daos-Lauenu apan Vasle Unves of aova aova ROMANIA
More information( ) () we define the interaction representation by the unitary transformation () = ()
Hgher Order Perurbaon Theory Mchael Fowler 3/7/6 The neracon Represenaon Recall ha n he frs par of hs course sequence, we dscussed he chrödnger and Hesenberg represenaons of quanum mechancs here n he chrödnger
More informationTHIS PAGE DECLASSIFIED IAW EO IRIS u blic Record. Key I fo mation. Ma n: AIR MATERIEL COMM ND. Adm ni trative Mar ings.
T H S PA G E D E CLA SSFED AW E O 2958 RS u blc Recod Key fo maon Ma n AR MATEREL COMM ND D cumen Type Call N u b e 03 V 7 Rcvd Rel 98 / 0 ndexe D 38 Eneed Dae RS l umbe 0 0 4 2 3 5 6 C D QC d Dac A cesson
More informationajanuary't I11 F or,'.
',f,". ; q - c. ^. L.+T,..LJ.\ ; - ~,.,.,.,,,E k }."...,'s Y l.+ : '. " = /.. :4.,Y., _.,,. "-.. - '// ' 7< s k," ;< - " fn 07 265.-.-,... - ma/ \/ e 3 p~~f v-acecu ean d a e.eng nee ng sn ~yoo y namcs
More informationTHE EQUIVALENCE OF GRAM-SCHMIDT AND QR FACTORIZATION (page 227) Gram-Schmidt provides another way to compute a QR decomposition: n
HE EQUIVAENCE OF GRA-SCHID AND QR FACORIZAION (page 7 Ga-Schdt podes anothe way to copute a QR decoposton: n gen ectos,, K, R, Ga-Schdt detenes scalas j such that o + + + [ ] [ ] hs s a QR factozaton of
More informationTRANSIENTS. Lecture 5 ELEC-E8409 High Voltage Engineering
TRANSIENTS Lece 5 ELECE8409 Hgh Volage Engneeng TRANSIENT VOLTAGES A ansen even s a sholved oscllaon (sgnfcanly fase han opeang feqency) n a sysem cased by a sdden change of volage, cen o load. Tansen
More informationCptS 570 Machine Learning School of EECS Washington State University. CptS Machine Learning 1
ps 57 Machne Leann School of EES Washnon Sae Unves ps 57 - Machne Leann Assume nsances of classes ae lneal sepaable Esmae paamees of lnea dscmnan If ( - -) > hen + Else - ps 57 - Machne Leann lassfcaon
More informationNanoparticles. Educts. Nucleus formation. Nucleus. Growth. Primary particle. Agglomeration Deagglomeration. Agglomerate
ucs Nucleus Nucleus omaon cal supesauaon Mng o eucs, empeaue, ec. Pmay pacle Gowh Inegaon o uson-lme pacle gowh Nanopacles Agglomeaon eagglomeaon Agglomeae Sablsaon o he nanopacles agans agglomeaon! anspo
More informationMethod of Characteristics for Pure Advection By Gilberto E. Urroz, September 2004
Mehod of Charaerss for Pre Adveon By Glbero E Urroz Sepember 004 Noe: The followng noes are based on lass noes for he lass COMPUTATIONAL HYDAULICS as agh by Dr Forres Holly n he Sprng Semeser 985 a he
More informationMATHEMATICAL FOUNDATIONS FOR APPROXIMATING PARTICLE BEHAVIOUR AT RADIUS OF THE PLANCK LENGTH
Fundamenal Jounal of Mahemaical Phsics Vol 3 Issue 013 Pages 55-6 Published online a hp://wwwfdincom/ MATHEMATICAL FOUNDATIONS FOR APPROXIMATING PARTICLE BEHAVIOUR AT RADIUS OF THE PLANCK LENGTH Univesias
More informationFast Calibration for Robot Welding System with Laser Vision
Fas Calbaon fo Robo Weldng Ssem h Lase Vson Lu Su Mechancal & Eleccal Engneeng Nanchang Unves Nanchang, Chna Wang Guoong Mechancal Engneeng Souh Chna Unves of echnolog Guanghou, Chna Absac Camea calbaon
More informationSpecial Relativity in Acoustic and Electromagnetic Waves Without Phase Invariance and Lorentz Transformations 1. Introduction n k.
Speial Relativit in Aousti and Eletomagneti Waves Without Phase Invaiane and Loentz Tansfomations Benhad Rothenstein bothenstein@gmail.om Abstat. Tansfomation equations fo the phsial quantities intodued
More informationChapter 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 informationPHY2053 Summer C 2013 Exam 1 Solutions
PHY053 Sue C 03 E Soluon. The foce G on o G G The onl cobnon h e '/ = doubln.. The peed of lh le 8fulon c 86,8 le 60 n 60n h 4h d 4d fonh.80 fulon/ fonh 3. The dnce eled fo he ene p,, 36 (75n h 45 The
More informationLecture 5. Plane Wave Reflection and Transmission
Lecue 5 Plane Wave Reflecon and Tansmsson Incden wave: 1z E ( z) xˆ E (0) e 1 H ( z) yˆ E (0) e 1 Nomal Incdence (Revew) z 1 (,, ) E H S y (,, ) 1 1 1 Refleced wave: 1z E ( z) xˆ E E (0) e S H 1 1z H (
More informationToday - Lecture 13. Today s lecture continue with rotations, torque, Note that chapters 11, 12, 13 all involve rotations
Today - Lecue 13 Today s lecue coninue wih oaions, oque, Noe ha chapes 11, 1, 13 all inole oaions slide 1 eiew Roaions Chapes 11 & 1 Viewed fom aboe (+z) Roaional, o angula elociy, gies angenial elociy
More informationThe Feigel Process. The Momentum of Quantum Vacuum. Geert Rikken Vojislav Krstic. CNRS-France. Ariadne call A0/1-4532/03/NL/MV 04/1201
The Fegel Pocess The Momenum of Quanum Vacuum a an Tggelen CNRS -Fance Laboaoe e Physque e Moélsaon es Mleux Complexes Unesé Joseph Foue/CNRS, Genoble, Fance Gee Ren Vosla Ksc CNRS Fance CNRS-Fance Laboaoe
More informationThe Impact of the Earth s Movement through the Space on Measuring the Velocity of Light (Part Two)
Jonal of Applied Mahemais and Phsis, 7, 5, 74-757 hp://wwwsipog/jonal/jamp ISSN Online: 7-479 ISSN Pin: 7-45 The Impa of he Eah s Movemen hogh he Spae on Measing he Veloi of Ligh (Pa Two Miloš Čojanović
More informationNotes on the stability of dynamic systems and the use of Eigen Values.
Noes on he sabl of dnamc ssems and he use of Egen Values. Source: Macro II course noes, Dr. Davd Bessler s Tme Seres course noes, zarads (999) Ineremporal Macroeconomcs chaper 4 & Techncal ppend, and Hamlon
More informationElectromagnetic waves in vacuum.
leromagne waves n vauum. The dsovery of dsplaemen urrens enals a peular lass of soluons of Maxwell equaons: ravellng waves of eler and magne felds n vauum. In he absene of urrens and harges, he equaons
More informationTWO INTERFACIAL COLLINEAR GRIFFITH CRACKS IN THERMO- ELASTIC COMPOSITE MEDIA
WO INERFIL OLLINER GRIFFIH RS IN HERMO- ELSI OMOSIE MEDI h m MISHR S DS * Deme o Mheml See I Ie o eholog BHU V-5 I he oee o he le o he e e o eeg o o olle Gh e he ee o he wo ohoo mel e e e emee el. he olem
More information2 shear strain / L for small angle
Sac quaons F F M al Sess omal sess foce coss-seconal aea eage Shea Sess shea sess shea foce coss-seconal aea llowable Sess Faco of Safe F. S San falue Shea San falue san change n lengh ognal lengh Hooke
More informationChapter Eight Notes N P U1C8S4-6
Chapte Eight Notes N P UC8S-6 Name Peiod Section 8.: Tigonometic Identities An identit is, b definition, an equation that is alwas tue thoughout its domain. B tue thoughout its domain, that is to sa that
More informationParameterization in large-scale atmospheric modelling
Paameeaon n lage-sale amose modellng Geneal aameeaon oblem: Ealaon of ems nolng aeaged qada and ge ode ods of nesoled deaons fom lage-sale aables Examles: a blen ansfe n e bonday laye b Effes of nesoled
More informationPhotographing a time interval
Potogaping a time inteval Benad Rotenstein and Ioan Damian Politennia Univesity of imisoaa Depatment of Pysis imisoaa Romania benad_otenstein@yaoo.om ijdamian@yaoo.om Abstat A metod of measuing time intevals
More informationMechanics Physics 151
Mechancs Physcs 5 Lecure 9 Hamlonan Equaons of Moon (Chaper 8) Wha We Dd Las Tme Consruced Hamlonan formalsm H ( q, p, ) = q p L( q, q, ) H p = q H q = p H = L Equvalen o Lagrangan formalsm Smpler, bu
More informationFinal Exam. Tuesday, December hours, 30 minutes
an Faniso ae Univesi Mihael Ba ECON 30 Fall 04 Final Exam Tuesda, Deembe 6 hous, 30 minues Name: Insuions. This is losed book, losed noes exam.. No alulaos of an kind ae allowed. 3. how all he alulaions.
More informationOH BOY! Story. N a r r a t iv e a n d o bj e c t s th ea t e r Fo r a l l a g e s, fr o m th e a ge of 9
OH BOY! O h Boy!, was or igin a lly cr eat ed in F r en ch an d was a m a jor s u cc ess on t h e Fr en ch st a ge f or young au di enc es. It h a s b een s een by ap pr ox i ma t ely 175,000 sp ect at
More informationIn electrostatics, the electric field E and its sources (charges) are related by Gauss s law: Surface
Ampee s law n eletostatis, the eleti field E and its soues (hages) ae elated by Gauss s law: EdA i 4πQenl Sufae Why useful? When symmety applies, E an be easily omputed Similaly, in magnetism the magneti
More information( ) ( ) Weibull Distribution: k ti. u u. Suppose t 1, t 2, t n are times to failure of a group of n mechanisms. The likelihood function is
Webll Dsbo: Des Bce Dep of Mechacal & Idsal Egeeg The Uvesy of Iowa pdf: f () exp Sppose, 2, ae mes o fale of a gop of mechasms. The lelhood fco s L ( ;, ) exp exp MLE: Webll 3//2002 page MLE: Webll 3//2002
More informationClassification of Equations Characteristics
Clssiiion o Eqions Cheisis Consie n elemen o li moing in wo imensionl spe enoe s poin P elow. The ph o P is inie he line. The posiion ile is s so h n inemenl isne long is s. Le he goening eqions e epesene
More informationFIRMS IN THE TWO-PERIOD FRAMEWORK (CONTINUED)
FIRMS IN THE TWO-ERIO FRAMEWORK (CONTINUE) OCTOBER 26, 2 Model Sucue BASICS Tmelne of evens Sa of economc plannng hozon End of economc plannng hozon Noaon : capal used fo poducon n peod (decded upon n
More informationMechanics Physics 151
Mechancs Physcs 5 Lecure 9 Hamlonan Equaons of Moon (Chaper 8) Wha We Dd Las Tme Consruced Hamlonan formalsm Hqp (,,) = qp Lqq (,,) H p = q H q = p H L = Equvalen o Lagrangan formalsm Smpler, bu wce as
More informationScalars and Vectors Scalar
Scalas and ectos Scala A phscal quantt that s completel chaacteed b a eal numbe (o b ts numecal value) s called a scala. In othe wods a scala possesses onl a magntude. Mass denst volume tempeatue tme eneg
More informationEE 410/510: Electromechanical Systems Chapter 3
EE 4/5: Eleomehnl Syem hpe 3 hpe 3. Inoon o Powe Eleon Moelng n Applon of Op. Amp. Powe Amplfe Powe onvee Powe Amp n Anlog onolle Swhng onvee Boo onvee onvee Flyb n Fow onvee eonn n Swhng onvee 5// All
More informationIn accordance with Regulation 21(1), the Agency has notified, and invited submissions &om, certain specified
hef xeuve Offe Wesen Regonal Fshees Boad The We odge al s odge Galway 6 June 2009 Re Dea S nvonmenal Poeon Ageny An Ghnwmhomoh un Oloomhnll omhshd Headquaes. PO Box 000 Johnsown asle sae ouny Wexfod, eland
More informationCombinatorial Approach to M/M/1 Queues. Using Hypergeometric Functions
Inenaional Mahemaical Foum, Vol 8, 03, no 0, 463-47 HIKARI Ld, wwwm-hikaicom Combinaoial Appoach o M/M/ Queues Using Hypegeomeic Funcions Jagdish Saan and Kamal Nain Depamen of Saisics, Univesiy of Delhi,
More informationMethods of Improving Constitutive Equations
Mehods o mprovng Consuve Equaons Maxell Model e an mprove h ne me dervaves or ne sran measures. ³ ª º «e, d» ¼ e an also hange he bas equaon lnear modaons non-lnear modaons her Consuve Approahes Smple
More informationPHYS-3301 Lecture 2. Aug. 31, How Small. is Small? How Fast is Fast? Structure of the course Modern Physics. Relativistic
Quantum (1920 s-) quantum (1927-) PHYS-3301 Lectue 2 Classical phsics Newtonian Mechanics, Themodnamics Statistical Mechanics, El.-Mag. (1905) Mawell s Equations of electomagnetism (1873) Aug. 31, 2017
More informationOutline. GW approximation. Electrons in solids. The Green Function. Total energy---well solved Single particle excitation---under developing
Peenaon fo Theoecal Condened Mae Phyc n TU Beln Geen-Funcon and GW appoxmaon Xnzheng L Theoy Depamen FHI May.8h 2005 Elecon n old Oulne Toal enegy---well olved Sngle pacle excaon---unde developng The Geen
More informationChapter 6 Plane Motion of Rigid Bodies
Chpe 6 Pne oon of Rd ode 6. Equon of oon fo Rd bod. 6., 6., 6.3 Conde d bod ced upon b ee een foce,, 3,. We cn ume h he bod mde of e numbe n of pce of m Δm (,,, n). Conden f he moon of he m cene of he
More informationChapter 5. Long Waves
ape 5. Lo Waes Wae e s o compaed ae dep: < < L π Fom ea ae eo o s s ; amos ozoa moo z p s ; dosac pesse Dep-aeaed coseao o mass
More informationChapter Lagrangian Interpolation
Chaper 5.4 agrangan Inerpolaon Afer readng hs chaper you should be able o:. dere agrangan mehod of nerpolaon. sole problems usng agrangan mehod of nerpolaon and. use agrangan nerpolans o fnd deraes and
More information(conservation of momentum)
Dynamis of Binay Collisions Assumptions fo elasti ollisions: a) Eletially neutal moleules fo whih the foe between moleules depends only on the distane between thei entes. b) No intehange between tanslational
More informationOrthotropic Materials
Kapiel 2 Ohoopic Maeials 2. Elasic Sain maix Elasic sains ae elaed o sesses by Hooke's law, as saed below. The sesssain elaionship is in each maeial poin fomulaed in he local caesian coodinae sysem. ε
More information( ) exp i ω b ( ) [ III-1 ] exp( i ω ab. exp( i ω ba
THE INTEACTION OF ADIATION AND MATTE: SEMICLASSICAL THEOY PAGE 26 III. EVIEW OF BASIC QUANTUM MECHANICS : TWO -LEVEL QUANTUM SYSTEMS : The lieaue of quanum opics and lase specoscop abounds wih discussions
More informationReflection and Refraction
Chape 3 Refleon and Refaon As we know fom eveyday expeene, when lgh aves a an nefae beween maeals paally efles and paally ansms. In hs hape, we examne wha happens o plane waves when hey popagae fom one
More informationCONSISTENT EARTHQUAKE ACCELERATION AND DISPLACEMENT RECORDS
APPENDX J CONSSTENT EARTHQUAKE ACCEERATON AND DSPACEMENT RECORDS Earhqake Acceleraons can be Measred. However, Srcres are Sbjeced o Earhqake Dsplacemens J. NTRODUCTON { XE "Acceleraon Records" }A he presen
More informationP a g e 5 1 of R e p o r t P B 4 / 0 9
P a g e 5 1 of R e p o r t P B 4 / 0 9 J A R T a l s o c o n c l u d e d t h a t a l t h o u g h t h e i n t e n t o f N e l s o n s r e h a b i l i t a t i o n p l a n i s t o e n h a n c e c o n n e
More informationTHE PHYSICS BEHIND THE SODACONSTRUCTOR. by Jeckyll
THE PHYSICS BEHIND THE SODACONSTRUCTOR b Jeckll THE PHYSICS BEHIND THE SODACONSTRUCTOR - b Jeckll /3 CONTENTS. INTRODUCTION 5. UNITS OF MEASUREMENT 7 3. DETERMINATION OF THE PHYSICAL CONSTANTS ADOPTED
More informationScienceDirect. Behavior of Integral Curves of the Quasilinear Second Order Differential Equations. Alma Omerspahic *
Avalable onlne a wwwscencedeccom ScenceDec oceda Engneeng 69 4 85 86 4h DAAAM Inenaonal Smposum on Inellgen Manufacung and Auomaon Behavo of Inegal Cuves of he uaslnea Second Ode Dffeenal Equaons Alma
More informationSet of square-integrable function 2 L : function space F
Set of squae-ntegable functon L : functon space F Motvaton: In ou pevous dscussons we have seen that fo fee patcles wave equatons (Helmholt o Schödnge) can be expessed n tems of egenvalue equatons. H E,
More informationMechanics Physics 151
Mechancs Physcs 5 Lecure 0 Canoncal Transformaons (Chaper 9) Wha We Dd Las Tme Hamlon s Prncple n he Hamlonan formalsm Dervaon was smple δi δ Addonal end-pon consrans pq H( q, p, ) d 0 δ q ( ) δq ( ) δ
More informationChapter 7. Interference
Chape 7 Inefeence Pa I Geneal Consideaions Pinciple of Supeposiion Pinciple of Supeposiion When wo o moe opical waves mee in he same locaion, hey follow supeposiion pinciple Mos opical sensos deec opical
More informationPolarization Basics E. Polarization Basics The equations
Plazan Ba he equan [ ω δ ] [ ω δ ] eeen a a f lane wave: he w mnen f he eleal feld f an wave agang n he z den, n neeal mnhma. he amlude, and hae δ, fluuae lwl wh ee he ad llan f he ae ω. z Plazan Ba [
More informationModal Analysis of Periodically Time-varying Linear Rotor Systems using Floquet Theory
7h IFoMM-Confeene on Roo Dynams Venna Ausa 25-28 Sepembe 2006 Modal Analyss of Peodally me-vayng Lnea Roo Sysems usng Floque heoy Chong-Won Lee Dong-Ju an Seong-Wook ong Cene fo Nose and Vbaon Conol (NOVIC)
More informationChapters 2 Kinematics. Position, Distance, Displacement
Chapers Knemacs Poson, Dsance, Dsplacemen Mechancs: Knemacs and Dynamcs. Knemacs deals wh moon, bu s no concerned wh he cause o moon. Dynamcs deals wh he relaonshp beween orce and moon. The word dsplacemen
More informationAvailable online Journal of Scientific and Engineering Research, 2017, 4(2): Research Article
Avlble onlne www.jse.com Jonl of Scenfc nd Engneeng Resech, 7, 4():5- Resech Acle SSN: 394-63 CODEN(USA): JSERBR Exc Solons of Qselsc Poblems of Lne Theoy of Vscoelscy nd Nonlne Theoy Vscoelscy fo echnclly
More information( ) α is determined to be a solution of the one-dimensional minimization problem: = 2. min = 2
Homewo (Patal Solton) Posted on Mach, 999 MEAM 5 Deental Eqaton Methods n Mechancs. Sole the ollowng mat eqaton A b by () Steepest Descent Method and/o Pecondtoned SD Method Snce the coecent mat A s symmetc,
More information