Using hypothesis one, energy of gravitational waves is directly proportional to its frequency,

Size: px
Start display at page:

Download "Using hypothesis one, energy of gravitational waves is directly proportional to its frequency,"

Transcription

1 ushl nd Grviy Prshn Shool of Siene nd ngineering, Universiy of Glsgow, Glsgow-G18QQ, Unied ingdo. * orresponding uhor: : Prshn. Shool of Siene nd ngineering, Universiy of Glsgow, Glsgow-G18QQ, Unied ingdo, Tel: ; -il: Prshn.9410@gil.o. Reeived: Deeber 08, 017; Aeped: Jnury 03, 018; Published: Jnury 10, 018 Absr nergy of grviionl wves is lwys qunized in for of is ngulr oenu. Bsed on hypohesis, vrible, ushl onsn is inrodued s i is onsn for given ss. Using his, he of grviionl wves rvelling in ss nd in spe-ie ws derived respeively. A loophole bsed on hypohesis ws used in deriving he equions of onsiousness whih hold rue for insein s ss-energy equivlene [1]. Definiion of grviy hs been redefined nd foruls for ie nd enropy in he for of ushl onsn were luled. eywords: Grviionl wves; Qunised; ushl onsn; quions of onsiousness; Mssenergy equivlene; Tie nd enropy Inroduion Hypohesis one, whenever n obje hnges is relive posiion in spe-ie, i rdies grviionl wves in he direion of oion nd his hnge is opposed by he effeive surrounding grviionl wves, obje ould be nyhing rnging fro n o o blk hole. Hypohesis wo, he origin of grviionl wves is lwys fro he enre of grviy of n obje. Hypohesis hree, grviionl wves rvels in srigh line. Qunized grviionl wves Using hypohesis one, energy of grviionl wves is direly proporionl o is frequeny, GW f Reoving proporionliy onsn, GW = f (1) Where is ushl onsn, deerined s follows: Fore of grviy in beween wo objes is given by iion: Prshn. ushl nd Grviy. J Phys Asron. 018; 6(1): Trde Siene In. 1

2 Jnury-018 G1 F [] lso Newon s seond lw of oion sys F=g [3], hene, i n be inferred h we ge g G g G, provided 1 = =. Also, for insein s ss-energy equivlene, Sine he energy of phoons is lwys qunised, = hf [4], hene i n be inferred h insein s ss-energy equivlene, we ge opring his resul wih equion 1, we ge Ghf g Gh g () Ghf g Agin, using If G = g, hen = h; where, is ushl onsn, is he ss of n obje, G is grviionl onsn, h is plnk s onsn, g is elerion due o grviy nd is he xiu veril disne fro he enre of grviy of n obje. ushl onsn hs been disussed in ler seions. Speed of GWs in ss onsider spheril obje res hving ss () nd rdius (). Using hypohesis wo, by equions of oion [5], v = u + g or v = g, sine obje is res. Where, v is he of GWs, g is elerion due o grviy nd is ie ken by GWs o rvel fro he enre o he periphery of ss. Hene, Speed g f (3) Sine energy of grviionl wves is lwys qunized, lso, poenil energy [6] he enre of he sphere is given by = g. Using equion 1 g k f Fro equion 3, i n be inferred h = / Using equion, beoes Gh 3 g (4) where G is grviionl onsn, h is plnk s onsn nd g is elerion due o grviy. G Fro Newonin grviy [],. Fro qunizion of energy, h f, nd fro poenil energy, g

3 Jnury-018. Puing he vlues of G, h nd g ino equion 4, we ge f Using insein s ss-energy equivlene, f bu lso Hene or f (5) or f (6) The of grviionl wves rvelling in ss is i.e. he of ligh. Speed of GWs in spe-ie onsider wo objes of idenil ss () nd rdius () in osi dne, eh hving n enngled phoon righ he enre while boh objes re inining disne of wih eh oher, is equl o he Shwrzshild rdius [7], given by G Newonin grviy, lso fro insein s ss-energy equivlene, G hene i n be foruled s: G By we ge = = 1 or 1 = 0. These re known s equions of onsiousness in ers of eleporion nd qunu enngleen respeively, whih is disussed in ler seions. Using equion 6, = f 1, fer pplying equion of onsiousness for qunu enngleen, 1=0, we ge, = f, sine qunu enngleen is independen of disne. Also, equion 5 n be rewrien s = f 1, using equion of onsiousness for eleporion, =1, = f or ff, his is due o he diffrion of GWs when hey ross he periphery of ss nd ener ino speie whih is nlogous o diffrion of ligh [8]. Using = f nd equion 6, we ge, =. Hene qunu eleporion is breking he singulriy nd he of grviionl wves rvelling in spe-ie is, or of he order of Th is why in reen deeion of GWs, GW170817, grviionl wves deviion fro he of ligh ws less hn few prs in Defining ushl Using hypohesis one nd hree, he erh is iled 3.4 o wih respe o he sun, o ke i siple only erh s roion in erin plne is ken ino onsiderion, i us be rdiing grviionl wves his ngle while he effeive surrounding grviionl wves re oing fro he sun n ngle of 0 o. A web of infinie nd inresing qudrilerls will be reed in beween he whih n be pproxied s prllelogr over shor disne nd his one prllelogr is one ushl. Moreover, his web is known s he grviy of he erh. onsn, ushl is defined in ers of ie nd enropy or he. 3

4 Jnury-018 Tie Speed of GWs in ss is whih n be wrien s on equing while using equion 1, (7) k king squres on boh sides,. Where Where is ie, is ss, is xiu veril disne fro enre of grviy of n obje nd is ushl onsn. I n be inferred h ie nd ushl onsn re inversely proporionl o eh oher; s we ove wy fro erh, he size of ushl inreses, hene ie srs flowing fser s opred o h on erh. nropy Fro equion, using diensions i n be inferred, kg k s Dividing by T on boh sides, we ge k J T where J/ is enropy (S), using equion 7, we ge S T opring i wih he lws of herodynis, whih sys Q Q S T, hene, where Q is he he bsorbed or relesed nd is xiu veril disne fro enre of grviy of n obje. quions of onsiousness =1 is he equion of onsiousness for eleporion nd i signifies insein s ss-energy equivlene. Le us ry i ou. Newon s lw of oion sys, F = g, lso Newonin grviy sys, F G on equing he, we ge, G = g (8). Fro Shwrzshild rdius, nd fro poenil energy 1 G g Using equion 8 in obinion wih =1, we will ge =. quion of onsiousness for eleporion is vlid proof of insein s ss-energy equivlene. Also, hese equions n only be used ording o he resonble will of onsious ind. onlusion nergy of grviionl wves is lwys qunised in for of is ngulr oenu. Speed of GWs rvelling in ss nd in speie is nd respeively. Foruls for ie nd enropy re derived in ers of ushl onsn. =1 is he 4

5 Jnury-018 equion of onsiousness for eleporion whih signifies ss-energy equivlene. Also, n ep hs been de o redefine grviy of n obje. RFRNS 1. Jenshel, Mihel. insein s ss-energy equivlene priniple. Aess Siene Poisson, Will M. Foundions of Newonin grviy. Grviy. 014; Murdin P. Newon s Lws of Moion. The nylopedi of Asronoy nd Asrophysis. 000; Sephenson L. Qunision of energy. Journl of he Insiuion of leril ngineers, 1963; Blkwell. quion of Moion. Dynis of Sruures. 013; Book. Poenil nergy Trnsfor. Risk Mngeen Shelon JD. Siple Inerpreion of he Shwrzshild Rdius. Aerin Journl of Physis. 1973; 41: Beeson S, Myer JW. Diffrion nd Inerferene. Perns of Ligh. 1987;

Three Dimensional Coordinate Geometry

Three Dimensional Coordinate Geometry HKCWCC dvned evel Pure Mhs. / -D Co-Geomer Three Dimensionl Coordine Geomer. Coordine of Poin in Spe Z XOX, YOY nd ZOZ re he oordine-es. P,, is poin on he oordine plne nd is lled ordered riple. P,, X Y

More information

P441 Analytical Mechanics - I. Coupled Oscillators. c Alex R. Dzierba

P441 Analytical Mechanics - I. Coupled Oscillators. c Alex R. Dzierba Lecure 3 Mondy - Deceber 5, 005 Wrien or ls upded: Deceber 3, 005 P44 Anlyicl Mechnics - I oupled Oscillors c Alex R. Dzierb oupled oscillors - rix echnique In Figure we show n exple of wo coupled oscillors,

More information

Motion. Part 2: Constant Acceleration. Acceleration. October Lab Physics. Ms. Levine 1. Acceleration. Acceleration. Units for Acceleration.

Motion. Part 2: Constant Acceleration. Acceleration. October Lab Physics. Ms. Levine 1. Acceleration. Acceleration. Units for Acceleration. Moion Accelerion Pr : Consn Accelerion Accelerion Accelerion Accelerion is he re of chnge of velociy. = v - vo = Δv Δ ccelerion = = v - vo chnge of velociy elpsed ime Accelerion is vecor, lhough in one-dimensionl

More information

Forms of Energy. Mass = Energy. Page 1. SPH4U: Introduction to Work. Work & Energy. Particle Physics:

Forms of Energy. Mass = Energy. Page 1. SPH4U: Introduction to Work. Work & Energy. Particle Physics: SPH4U: Inroducion o ork ork & Energy ork & Energy Discussion Definiion Do Produc ork of consn force ork/kineic energy heore ork of uliple consn forces Coens One of he os iporn conceps in physics Alernive

More information

September 20 Homework Solutions

September 20 Homework Solutions College of Engineering nd Compuer Science Mechnicl Engineering Deprmen Mechnicl Engineering A Seminr in Engineering Anlysis Fll 7 Number 66 Insrucor: Lrry Creo Sepember Homework Soluions Find he specrum

More information

Physics 2A HW #3 Solutions

Physics 2A HW #3 Solutions Chper 3 Focus on Conceps: 3, 4, 6, 9 Problems: 9, 9, 3, 41, 66, 7, 75, 77 Phsics A HW #3 Soluions Focus On Conceps 3-3 (c) The ccelerion due o grvi is he sme for boh blls, despie he fc h he hve differen

More information

A Closed Model of the Universe

A Closed Model of the Universe Inernionl Journl of Asronomy nd Asrophysis 03 3 89-98 hp://dxdoiorg/036/ij0330 Published Online June 03 (hp://wwwsirporg/journl/ij) A Closed Model of he Universe Fdel A Bukhri Deprn of Asronomy Fuly of

More information

Cylindrically Symmetric Marder Universe and Its Proper Teleparallel Homothetic Motions

Cylindrically Symmetric Marder Universe and Its Proper Teleparallel Homothetic Motions J. Bsi. Appl. i. Res. 4-5 4 4 TeRod Publiion IN 9-44 Journl of Bsi nd Applied ienifi Reserh www.erod.om Clindrill mmeri Mrder Universe nd Is Proper Teleprllel Homohei Moions Amjd Ali * Anwr Ali uhil Khn

More information

Version 001 test-1 swinney (57010) 1. is constant at m/s.

Version 001 test-1 swinney (57010) 1. is constant at m/s. Version 001 es-1 swinne (57010) 1 This prin-ou should hve 20 quesions. Muliple-choice quesions m coninue on he nex column or pge find ll choices before nswering. CubeUniVec1x76 001 10.0 poins Acubeis1.4fee

More information

A Kalman filtering simulation

A Kalman filtering simulation A Klmn filering simulion The performnce of Klmn filering hs been esed on he bsis of wo differen dynmicl models, ssuming eiher moion wih consn elociy or wih consn ccelerion. The former is epeced o beer

More information

Chapter 10. Simple Harmonic Motion and Elasticity. Goals for Chapter 10

Chapter 10. Simple Harmonic Motion and Elasticity. Goals for Chapter 10 Chper 0 Siple Hronic Moion nd Elsiciy Gols or Chper 0 o ollow periodic oion o sudy o siple hronic oion. o sole equions o siple hronic oion. o use he pendulu s prooypicl syse undergoing siple hronic oion.

More information

Think of the Relationship Between Time and Space Again

Think of the Relationship Between Time and Space Again Repor nd Opinion, 1(3),009 hp://wwwsciencepubne sciencepub@gmilcom Think of he Relionship Beween Time nd Spce Agin Yng F-cheng Compny of Ruid Cenre in Xinjing 15 Hongxing Sree, Klmyi, Xingjing 834000,

More information

2D Motion WS. A horizontally launched projectile s initial vertical velocity is zero. Solve the following problems with this information.

2D Motion WS. A horizontally launched projectile s initial vertical velocity is zero. Solve the following problems with this information. Nme D Moion WS The equions of moion h rele o projeciles were discussed in he Projecile Moion Anlsis Acii. ou found h projecile moes wih consn eloci in he horizonl direcion nd consn ccelerion in he ericl

More information

Energy Momentum Tensor for Photonic System

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

More information

2.3 The Lorentz Transformation Eq.

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

More information

e t dt e t dt = lim e t dt T (1 e T ) = 1

e t dt e t dt = lim e t dt T (1 e T ) = 1 Improper Inegrls There re wo ypes of improper inegrls - hose wih infinie limis of inegrion, nd hose wih inegrnds h pproch some poin wihin he limis of inegrion. Firs we will consider inegrls wih infinie

More information

ANSWERS TO EVEN NUMBERED EXERCISES IN CHAPTER 2

ANSWERS TO EVEN NUMBERED EXERCISES IN CHAPTER 2 ANSWERS TO EVEN NUMBERED EXERCISES IN CHAPTER Seion Eerise -: Coninuiy of he uiliy funion Le λ ( ) be he monooni uiliy funion defined in he proof of eisene of uiliy funion If his funion is oninuous y hen

More information

An object moving with speed v around a point at distance r, has an angular velocity. m/s m

An object moving with speed v around a point at distance r, has an angular velocity. m/s m Roion The mosphere roes wih he erh n moions wihin he mosphere clerly follow cure phs (cyclones, nicyclones, hurricnes, ornoes ec.) We nee o epress roion quniiely. For soli objec or ny mss h oes no isor

More information

The Forming Theory and Computer Simulation of the Rotary Cutting Tools with Helical Teeth and Complex Surfaces

The Forming Theory and Computer Simulation of the Rotary Cutting Tools with Helical Teeth and Complex Surfaces Compuer nd Informion Siene The Forming Theory nd Compuer Simulion of he Rory Cuing Tools wih Helil Teeh nd Comple Surfes Hurn Liu Deprmen of Mehnil Engineering Zhejing Universiy of Siene nd Tehnology Hngzhou

More information

Generalized The General Relativity Using Generalized Lorentz Transformation

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

More information

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

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

More information

The solution is often represented as a vector: 2xI + 4X2 + 2X3 + 4X4 + 2X5 = 4 2xI + 4X2 + 3X3 + 3X4 + 3X5 = 4. 3xI + 6X2 + 6X3 + 3X4 + 6X5 = 6.

The solution is often represented as a vector: 2xI + 4X2 + 2X3 + 4X4 + 2X5 = 4 2xI + 4X2 + 3X3 + 3X4 + 3X5 = 4. 3xI + 6X2 + 6X3 + 3X4 + 6X5 = 6. [~ o o :- o o ill] i 1. Mrices, Vecors, nd Guss-Jordn Eliminion 1 x y = = - z= The soluion is ofen represened s vecor: n his exmple, he process of eliminion works very smoohly. We cn elimine ll enries

More information

Contraction Mapping Principle Approach to Differential Equations

Contraction Mapping Principle Approach to Differential Equations epl Journl of Science echnology 0 (009) 49-53 Conrcion pping Principle pproch o Differenil Equions Bishnu P. Dhungn Deprmen of hemics, hendr Rn Cmpus ribhuvn Universiy, Khmu epl bsrc Using n eension of

More information

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

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

More information

STUDY OF THERMAL PROPERTIES OF POROUS MATERIALS

STUDY OF THERMAL PROPERTIES OF POROUS MATERIALS SUY OF HRMAL PROPRIS OF POROUS MARIALS Oldři Zeškl, Pvl Šefková Insiue of Pysil nd Alied Ceisry, Fuly of Ceisry, Brno Universiy of enology, Purkyňov 118, CZ-61 Brno, Cze Reubli il: zeskl@f.vubr.z, sefkov@f.vubr.z

More information

A1.1.1 Model for the vertical stress comparison between the FLAC ubiquitous joints model and the theoretical development in Jaeger and Cook (1979)

A1.1.1 Model for the vertical stress comparison between the FLAC ubiquitous joints model and the theoretical development in Jaeger and Cook (1979) Universiy of Preori ed Krprov, K (007) Appendix 1. FLAC models nd derivions APPEDIX 1. FLAC MODELS AD DEIATIOS A1.1 Applied models for FLAC ode A1.1.1 Model for he veril sress omprison beween he FLAC ubiquious

More information

PHYSICS 1210 Exam 1 University of Wyoming 14 February points

PHYSICS 1210 Exam 1 University of Wyoming 14 February points PHYSICS 1210 Em 1 Uniersiy of Wyoming 14 Februry 2013 150 poins This es is open-noe nd closed-book. Clculors re permied bu compuers re no. No collborion, consulion, or communicion wih oher people (oher

More information

A New Formulation of Electrodynamics

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

More information

A LOG IS AN EXPONENT.

A LOG IS AN EXPONENT. Ojeives: n nlze nd inerpre he ehvior of rihmi funions, inluding end ehvior nd smpoes. n solve rihmi equions nlill nd grphill. n grph rihmi funions. n deermine he domin nd rnge of rihmi funions. n deermine

More information

A 1.3 m 2.5 m 2.8 m. x = m m = 8400 m. y = 4900 m 3200 m = 1700 m

A 1.3 m 2.5 m 2.8 m. x = m m = 8400 m. y = 4900 m 3200 m = 1700 m PHYS : Soluions o Chper 3 Home Work. SSM REASONING The displcemen is ecor drwn from he iniil posiion o he finl posiion. The mgniude of he displcemen is he shores disnce beween he posiions. Noe h i is onl

More information

A cosmological view on Milgrom s acceleration constant

A cosmological view on Milgrom s acceleration constant Preprins (www.preprins.org NOT PEER-REVIEWED Posed: Deember 7 doi:.9/preprins7.77.v A osmologil view on Milgrom s elerion onsn Engel Roz Sripperwei, 555 ST Vlkenswrd, The Neherlnds Emil: engel.roz@onsbrbnne.nl

More information

two values, false and true used in mathematical logic, and to two voltage levels, LOW and HIGH used in switching circuits.

two values, false and true used in mathematical logic, and to two voltage levels, LOW and HIGH used in switching circuits. Digil Logi/Design. L. 3 Mrh 2, 26 3 Logi Ges nd Boolen Alger 3. CMOS Tehnology Digil devises re predominnly mnufured in he Complemenry-Mel-Oide-Semionduor (CMOS) ehnology. Two ypes of swihes, s disussed

More information

Computer Aided Geometric Design

Computer Aided Geometric Design Copue Aided Geoei Design Geshon Ele, Tehnion sed on ook Cohen, Riesenfeld, & Ele Geshon Ele, Tehnion Definiion 3. The Cile Given poin C in plne nd nue R 0, he ile ih ene C nd dius R is defined s he se

More information

4.8 Improper Integrals

4.8 Improper Integrals 4.8 Improper Inegrls Well you ve mde i hrough ll he inegrion echniques. Congrs! Unforunely for us, we sill need o cover one more inegrl. They re clled Improper Inegrls. A his poin, we ve only del wih inegrls

More information

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

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

More information

Motion in a Straight Line

Motion in a Straight Line Moion in Srigh Line. Preei reched he mero sion nd found h he esclor ws no working. She wlked up he sionry esclor in ime. On oher dys, if she remins sionry on he moing esclor, hen he esclor kes her up in

More information

Equations from The Four Principal Kinetic States of Material Bodies. Copyright 2005 Joseph A. Rybczyk

Equations from The Four Principal Kinetic States of Material Bodies. Copyright 2005 Joseph A. Rybczyk Equions fom he Fou Pinipl Kinei Ses of Meil Bodies Copyigh 005 Joseph A. Rybzyk Following is omplee lis of ll of he equions used in o deied in he Fou Pinipl Kinei Ses of Meil Bodies. Eh equion is idenified

More information

ME 141. Engineering Mechanics

ME 141. Engineering Mechanics ME 141 Engineeing Mechnics Lecue 13: Kinemics of igid bodies hmd Shhedi Shkil Lecue, ep. of Mechnicl Engg, UET E-mil: sshkil@me.bue.c.bd, shkil6791@gmil.com Websie: eche.bue.c.bd/sshkil Couesy: Veco Mechnics

More information

[5] Solving Multiple Linear Equations A system of m linear equations and n unknown variables:

[5] Solving Multiple Linear Equations A system of m linear equations and n unknown variables: [5] Solving Muliple Liner Equions A syse of liner equions nd n unknown vribles: + + + nn = b + + + = b n n : + + + nn = b n n A= b, where A =, : : : n : : : : n = : n A = = = ( ) where, n j = ( ); = :

More information

6. Gas dynamics. Ideal gases Speed of infinitesimal disturbances in still gas

6. Gas dynamics. Ideal gases Speed of infinitesimal disturbances in still gas 6. Gs dynmics Dr. Gergely Krisóf De. of Fluid echnics, BE Februry, 009. Seed of infiniesiml disurbnces in sill gs dv d, dv d, Coninuiy: ( dv)( ) dv omenum r r heorem: ( ( dv) ) d 3443 4 q m dv d dv llievi

More information

MTH 146 Class 11 Notes

MTH 146 Class 11 Notes 8.- Are of Surfce of Revoluion MTH 6 Clss Noes Suppose we wish o revolve curve C round n is nd find he surfce re of he resuling solid. Suppose f( ) is nonnegive funcion wih coninuous firs derivive on he

More information

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

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

More information

Armenian Theory of Special Relativity

Armenian Theory of Special Relativity renin Theory of Speil Reliiy ( Illusred) Rober Nzryn, & Hik Nzryn hysis Depren, Yeren Se Uniersiy, Yeren 005, reni hysis sronoy Depren, Cliforni Se Uniersiy, Norhridge, US bsr The i of his urren rile is

More information

LIGHT and SPECIAL RELATIVITY

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

More information

Derivation of the Missing Equations of Special Relativity from de-broglie s Matter Wave Concept and the Correspondence between Them

Derivation of the Missing Equations of Special Relativity from de-broglie s Matter Wave Concept and the Correspondence between Them Asian Journa of Aied Siene and Engineering, Voue, No /3 ISSN 35-95X(); 37-9584(e) Deriaion of he Missing Equaions of Seia Reaiiy fro de-brogie s Maer Wae Cone and he Corresondene beween The M.O.G. Taukder,

More information

A-B-Cs of Sun-Synchronous Orbit Mission Design

A-B-Cs of Sun-Synchronous Orbit Mission Design A-B-Cs of Sun-Synhronous Orbi Mission Design Ronald J. Boain Je Propulsion aboraory California nsiue of Tehnology AAS/AAA Spae Fligh Mehanis Conferene Maui, Hawaii 8-12 February 24 9 February 24 1 W S

More information

Magnetostatics Bar Magnet. Magnetostatics Oersted s Experiment

Magnetostatics Bar Magnet. Magnetostatics Oersted s Experiment Mgneosics Br Mgne As fr bck s 4500 yers go, he Chinese discovered h cerin ypes of iron ore could rc ech oher nd cerin mels. Iron filings "mp" of br mgne s field Crefully suspended slivers of his mel were

More information

Solutions to assignment 3

Solutions to assignment 3 D Sruure n Algorihm FR 6. Informik Sner, Telikeplli WS 03/04 hp://www.mpi-.mpg.e/~ner/oure/lg03/inex.hml Soluion o ignmen 3 Exerie Arirge i he ue of irepnie in urreny exhnge re o rnform one uni of urreny

More information

GeoTrig Notes Conventions and Notation: First Things First - Pythogoras and His Triangle. Conventions and Notation: GeoTrig Notes 04-14

GeoTrig Notes Conventions and Notation: First Things First - Pythogoras and His Triangle. Conventions and Notation: GeoTrig Notes 04-14 Convenions nd Noion: GeoTrig Noes 04-14 Hello ll, his revision inludes some numeri exmples s well s more rigonomery heory. This se of noes is inended o ompny oher uorils in his series: Inroduion o EDA,

More information

Physic 231 Lecture 4. Mi it ftd l t. Main points of today s lecture: Example: addition of velocities Trajectories of objects in 2 = =

Physic 231 Lecture 4. Mi it ftd l t. Main points of today s lecture: Example: addition of velocities Trajectories of objects in 2 = = Mi i fd l Phsic 3 Lecure 4 Min poins of od s lecure: Emple: ddiion of elociies Trjecories of objecs in dimensions: dimensions: g 9.8m/s downwrds ( ) g o g g Emple: A foobll pler runs he pern gien in he

More information

Average & instantaneous velocity and acceleration Motion with constant acceleration

Average & instantaneous velocity and acceleration Motion with constant acceleration Physics 7: Lecure Reminders Discussion nd Lb secions sr meeing ne week Fill ou Pink dd/drop form if you need o swich o differen secion h is FULL. Do i TODAY. Homework Ch. : 5, 7,, 3,, nd 6 Ch.: 6,, 3 Submission

More information

PARABOLA. moves such that PM. = e (constant > 0) (eccentricity) then locus of P is called a conic. or conic section.

PARABOLA. moves such that PM. = e (constant > 0) (eccentricity) then locus of P is called a conic. or conic section. wwwskshieducioncom PARABOLA Le S be given fixed poin (focus) nd le l be given fixed line (Direcrix) Le SP nd PM be he disnce of vrible poin P o he focus nd direcrix respecively nd P SP moves such h PM

More information

REAL ANALYSIS I HOMEWORK 3. Chapter 1

REAL ANALYSIS I HOMEWORK 3. Chapter 1 REAL ANALYSIS I HOMEWORK 3 CİHAN BAHRAN The quesions re from Sein nd Shkrchi s e. Chper 1 18. Prove he following sserion: Every mesurble funcion is he limi.e. of sequence of coninuous funcions. We firs

More information

M r. d 2. R t a M. Structural Mechanics Section. Exam CT5141 Theory of Elasticity Friday 31 October 2003, 9:00 12:00 hours. Problem 1 (3 points)

M r. d 2. R t a M. Structural Mechanics Section. Exam CT5141 Theory of Elasticity Friday 31 October 2003, 9:00 12:00 hours. Problem 1 (3 points) Delf Universiy of Technology Fculy of Civil Engineering nd Geosciences Srucurl echnics Secion Wrie your nme nd sudy numer he op righ-hnd of your work. Exm CT5 Theory of Elsiciy Fridy Ocoer 00, 9:00 :00

More information

Mocanu Paradox of Different Types of Lorentz Transformations

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

More information

Problem Set 9 Due December, 7

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

More information

The order of reaction is defined as the number of atoms or molecules whose concentration change during the chemical reaction.

The order of reaction is defined as the number of atoms or molecules whose concentration change during the chemical reaction. www.hechemisryguru.com Re Lw Expression Order of Recion The order of recion is defined s he number of oms or molecules whose concenrion chnge during he chemicl recion. Or The ol number of molecules or

More information

(1) (discrete choice) (inter-city mode choice) (1) (1) c m m. t m m β m β t. ε m (1) Ortúzar(1996) (shadow price)

(1) (discrete choice) (inter-city mode choice) (1) (1) c m m. t m m β m β t. ε m (1) Ortúzar(1996) (shadow price) 69-8 () 998 4 8 998 8 0 Orúzr(996) (disree hoie) (iner-iy mode hoie) m () m m m () m m m m β m β ε m () (996) Orúzr (shdow rie) 69 (). (). ( / ) () β β ε () () 70 () β = α β = α (4) (5) () (4) (5) () ()

More information

Some Inequalities variations on a common theme Lecture I, UL 2007

Some Inequalities variations on a common theme Lecture I, UL 2007 Some Inequliies vriions on common heme Lecure I, UL 2007 Finbrr Hollnd, Deprmen of Mhemics, Universiy College Cork, fhollnd@uccie; July 2, 2007 Three Problems Problem Assume i, b i, c i, i =, 2, 3 re rel

More information

Designing A Fanlike Structure

Designing A Fanlike Structure Designing A Fnlike Sruure To proeed wih his lesson, lik on he Nex buon here or he op of ny pge. When you re done wih his lesson, lik on he Conens buon here or he op of ny pge o reurn o he lis of lessons.

More information

3. Renewal Limit Theorems

3. Renewal Limit Theorems Virul Lborories > 14. Renewl Processes > 1 2 3 3. Renewl Limi Theorems In he inroducion o renewl processes, we noed h he rrivl ime process nd he couning process re inverses, in sens The rrivl ime process

More information

Proper Projective Symmetry in some well known Conformally flat Space-Times

Proper Projective Symmetry in some well known Conformally flat Space-Times roper rojeie Smmer in some well nown onformll fl Spe-Times Ghulm Shir Ful of Engineering Sienes GIK Insiue of Engineering Sienes nd Tehnolog Topi Swi NWF isn Emil: shir@gii.edu.p sr sud of onformll fl

More information

(b) 10 yr. (b) 13 m. 1.6 m s, m s m s (c) 13.1 s. 32. (a) 20.0 s (b) No, the minimum distance to stop = 1.00 km. 1.

(b) 10 yr. (b) 13 m. 1.6 m s, m s m s (c) 13.1 s. 32. (a) 20.0 s (b) No, the minimum distance to stop = 1.00 km. 1. Answers o Een Numbered Problems Chper. () 7 m s, 6 m s (b) 8 5 yr 4.. m ih 6. () 5. m s (b).5 m s (c).5 m s (d) 3.33 m s (e) 8. ().3 min (b) 64 mi..3 h. ().3 s (b) 3 m 4..8 mi wes of he flgpole 6. (b)

More information

0 for t < 0 1 for t > 0

0 for t < 0 1 for t > 0 8.0 Sep nd del funcions Auhor: Jeremy Orloff The uni Sep Funcion We define he uni sep funcion by u() = 0 for < 0 for > 0 I is clled he uni sep funcion becuse i kes uni sep = 0. I is someimes clled he Heviside

More information

Newtonian Relativity

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

More information

Chapter 12: Velocity, acceleration, and forces

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

More information

EXERCISE - 01 CHECK YOUR GRASP

EXERCISE - 01 CHECK YOUR GRASP UNIT # 09 PARABOLA, ELLIPSE & HYPERBOLA PARABOLA EXERCISE - 0 CHECK YOUR GRASP. Hin : Disnce beween direcri nd focus is 5. Given (, be one end of focl chord hen oher end be, lengh of focl chord 6. Focus

More information

Chapter 2. Motion along a straight line. 9/9/2015 Physics 218

Chapter 2. Motion along a straight line. 9/9/2015 Physics 218 Chper Moion long srigh line 9/9/05 Physics 8 Gols for Chper How o describe srigh line moion in erms of displcemen nd erge elociy. The mening of insnneous elociy nd speed. Aerge elociy/insnneous elociy

More information

Available Online :

Available Online : fo/u fopjr Hh# u] ugh vjehs de] foifr ns[ NsMs rqjr e/;e eu dj ';ea iq#" flg ldyi dj] lgrs foifr vusd] ^cu^ u NsMs /;s; ds] j?qcj j[s VsdAA jfpr% euo /ez iz.sr ln~xq# Jh j.nsmnlh egj STUDY PACKAGE Subjec

More information

2k 1. . And when n is odd number, ) The conclusion is when n is even number, an. ( 1) ( 2 1) ( k 0,1,2 L )

2k 1. . And when n is odd number, ) The conclusion is when n is even number, an. ( 1) ( 2 1) ( k 0,1,2 L ) Scholrs Journl of Engineering d Technology SJET) Sch. J. Eng. Tech., ; A):8-6 Scholrs Acdemic d Scienific Publisher An Inernionl Publisher for Acdemic d Scienific Resources) www.sspublisher.com ISSN -X

More information

INTEGRALS. Exercise 1. Let f : [a, b] R be bounded, and let P and Q be partitions of [a, b]. Prove that if P Q then U(P ) U(Q) and L(P ) L(Q).

INTEGRALS. Exercise 1. Let f : [a, b] R be bounded, and let P and Q be partitions of [a, b]. Prove that if P Q then U(P ) U(Q) and L(P ) L(Q). INTEGRALS JOHN QUIGG Eercise. Le f : [, b] R be bounded, nd le P nd Q be priions of [, b]. Prove h if P Q hen U(P ) U(Q) nd L(P ) L(Q). Soluion: Le P = {,..., n }. Since Q is obined from P by dding finiely

More information

a) Read over steps (1)- (4) below and sketch the path of the cycle on a P V plot on the graph below. Label all appropriate points.

a) Read over steps (1)- (4) below and sketch the path of the cycle on a P V plot on the graph below. Label all appropriate points. Prole 3: Crnot Cyle of n Idel Gs In this prole, the strting pressure P nd volue of n idel gs in stte, re given he rtio R = / > of the volues of the sttes nd is given Finlly onstnt γ = 5/3 is given You

More information

The Contradiction within Equations of Motion with Constant Acceleration

The Contradiction within Equations of Motion with Constant Acceleration The Conradicion wihin Equaions of Moion wih Consan Acceleraion Louai Hassan Elzein Basheir (Daed: July 7, 0 This paper is prepared o demonsrae he violaion of rules of mahemaics in he algebraic derivaion

More information

The Special Theory of Relativity

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

More information

THE 2-BODY PROBLEM. FIGURE 1. A pair of ellipses sharing a common focus. (c,b) c+a ROBERT J. VANDERBEI

THE 2-BODY PROBLEM. FIGURE 1. A pair of ellipses sharing a common focus. (c,b) c+a ROBERT J. VANDERBEI THE 2-BODY PROBLEM ROBERT J. VANDERBEI ABSTRACT. In his shor noe, we show ha a pair of ellipses wih a common focus is a soluion o he 2-body problem. INTRODUCTION. Solving he 2-body problem from scrach

More information

MM3 POE Solution Sheet Polymer Engineering. Q1. (a) CREEP RECOVERY STRESS RELAXATION

MM3 POE Solution Sheet Polymer Engineering. Q1. (a) CREEP RECOVERY STRESS RELAXATION Q1. () CREEP RECOVERY STRESS RELAXATION Mxwell ε σ Kelvin ε σ Sndrd Liner Solid ε σ Mxwell: Kelvin: SLS: Creep poor represenion of reep nd no ime dependen reovery Resonble relxion behviour, bu no residul

More information

Global alignment in linear space

Global alignment in linear space Globl linmen in liner spe 1 2 Globl linmen in liner spe Gol: Find n opiml linmen of A[1..n] nd B[1..m] in liner spe, i.e. O(n) Exisin lorihm: Globl linmen wih bkrkin O(nm) ime nd spe, bu he opiml os n

More information

Math 2142 Exam 1 Review Problems. x 2 + f (0) 3! for the 3rd Taylor polynomial at x = 0. To calculate the various quantities:

Math 2142 Exam 1 Review Problems. x 2 + f (0) 3! for the 3rd Taylor polynomial at x = 0. To calculate the various quantities: Mah 4 Eam Review Problems Problem. Calculae he 3rd Taylor polynomial for arcsin a =. Soluion. Le f() = arcsin. For his problem, we use he formula f() + f () + f ()! + f () 3! for he 3rd Taylor polynomial

More information

Physics 235 Chapter 2. Chapter 2 Newtonian Mechanics Single Particle

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

More information

f t f a f x dx By Lin McMullin f x dx= f b f a. 2

f t f a f x dx By Lin McMullin f x dx= f b f a. 2 Accumulion: Thoughs On () By Lin McMullin f f f d = + The gols of he AP* Clculus progrm include he semen, Sudens should undersnd he definie inegrl s he ne ccumulion of chnge. 1 The Topicl Ouline includes

More information

ECE Microwave Engineering. Fall Prof. David R. Jackson Dept. of ECE. Notes 10. Waveguides Part 7: Transverse Equivalent Network (TEN)

ECE Microwave Engineering. Fall Prof. David R. Jackson Dept. of ECE. Notes 10. Waveguides Part 7: Transverse Equivalent Network (TEN) EE 537-635 Microwve Engineering Fll 7 Prof. Dvid R. Jcson Dep. of EE Noes Wveguides Pr 7: Trnsverse Equivlen Newor (N) Wveguide Trnsmission Line Model Our gol is o come up wih rnsmission line model for

More information

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

PHYS-3301 Lecture 5. Chapter 2. Announcement. Sep. 12, Special Relativity. What about y and z coordinates? (x - direction of motion) Announemen Course webpage hp://www.phys.u.edu/~slee/33/ Tebook PHYS-33 Leure 5 HW (due 9/4) Chaper, 6, 36, 4, 45, 5, 5, 55, 58 Sep., 7 Chaper Speial Relaiiy. Basi Ideas. Consequenes of Einsein s Posulaes

More information

f(x) dx with An integral having either an infinite limit of integration or an unbounded integrand is called improper. Here are two examples dx x x 2

f(x) dx with An integral having either an infinite limit of integration or an unbounded integrand is called improper. Here are two examples dx x x 2 Impope Inegls To his poin we hve only consideed inegls f() wih he is of inegion nd b finie nd he inegnd f() bounded (nd in fc coninuous ecep possibly fo finiely mny jump disconinuiies) An inegl hving eihe

More information

Analysis of Tubular Linear Permanent Magnet Motor for Drilling Application

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

More information

Capacitance and Inductance. The Capacitor

Capacitance and Inductance. The Capacitor apaiane and Induane OUTINE apaiors apaior volage, urren, power, energy Induors eure 9, 9/9/5 Reading Hambley haper 3 (A) EE4 Fall 5 eure 9, Slide The apaior Two onduors (a,b) separaed by an insulaor: differene

More information

NEWTON S SECOND LAW OF MOTION

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

More information

Temperature Rise of the Earth

Temperature Rise of the Earth Avilble online www.sciencedirec.com ScienceDirec Procedi - Socil nd Behviorl Scien ce s 88 ( 2013 ) 220 224 Socil nd Behviorl Sciences Symposium, 4 h Inernionl Science, Socil Science, Engineering nd Energy

More information

April 8, 2017 Math 9. Geometry. Solving vector problems. Problem. Prove that if vectors and satisfy, then.

April 8, 2017 Math 9. Geometry. Solving vector problems. Problem. Prove that if vectors and satisfy, then. pril 8, 2017 Mth 9 Geometry Solving vetor prolems Prolem Prove tht if vetors nd stisfy, then Solution 1 onsider the vetor ddition prllelogrm shown in the Figure Sine its digonls hve equl length,, the prllelogrm

More information

Phys 110. Answers to even numbered problems on Midterm Map

Phys 110. Answers to even numbered problems on Midterm Map Phys Answers o een numbered problems on Miderm Mp. REASONING The word per indices rio, so.35 mm per dy mens.35 mm/d, which is o be epressed s re in f/cenury. These unis differ from he gien unis in boh

More information

Anatoly A. Kilbas. tn 1. t 1 a. dt 2. a t. log x

Anatoly A. Kilbas. tn 1. t 1 a. dt 2. a t. log x J. Koren Mh. So. 38 200) No. 6. 9 204 HADAMARD-TYPE FRACTIONAL CALCULUS Anoly A. Kilbs Absr. The er is devoed o he sudy of frionl inegrion nd differeniion on finie inervl [ b] of he rel xis in he frme

More information

An integral having either an infinite limit of integration or an unbounded integrand is called improper. Here are two examples.

An integral having either an infinite limit of integration or an unbounded integrand is called improper. Here are two examples. Improper Inegrls To his poin we hve only considered inegrls f(x) wih he is of inegrion nd b finie nd he inegrnd f(x) bounded (nd in fc coninuous excep possibly for finiely mny jump disconinuiies) An inegrl

More information

y z A left-handed system can be rotated to look like the following. z

y z A left-handed system can be rotated to look like the following. z Chpter 2 Crtesin Coördintes The djetive Crtesin bove refers to René Desrtes (1596 1650), who ws the first to oördintise the plne s ordered pirs of rel numbers, whih provided the first sstemti link between

More information

white strictly far ) fnf regular [ with f fcs)8( hs ) as function Preliminary question jointly speaking does not exist! Brownian : APA Lecture 1.

white strictly far ) fnf regular [ with f fcs)8( hs ) as function Preliminary question jointly speaking does not exist! Brownian : APA Lecture 1. Am : APA Lecure 13 Brownin moion Preliminry quesion : Wh is he equivlen in coninuous ime of sequence of? iid Ncqe rndom vribles ( n nzn noise ( 4 e Re whie ( ie se every fm ( xh o + nd covrince E ( xrxs

More information

Einstein s Derivation of the Lorentz Transformations in the1905 Paper is Internally Inconsistent

Einstein s Derivation of the Lorentz Transformations in the1905 Paper is Internally Inconsistent Einsein s Deriion of he Lorenz Trnsformions in he195 Pper is Inernlly Inonsisen Jon C. Freemn Absr The generl onsensus in lierure onerning Einsein s 195 pper on speil reliiy, is h he independenly deried

More information

Homework 2 Solutions

Homework 2 Solutions Mah 308 Differenial Equaions Fall 2002 & 2. See he las page. Hoework 2 Soluions 3a). Newon s secon law of oion says ha a = F, an we know a =, so we have = F. One par of he force is graviy, g. However,

More information

D zone schemes

D zone schemes Ch. 5. Enegy Bnds in Cysls 5.. -D zone schemes Fee elecons E k m h Fee elecons in cysl sinα P + cosα cosk α cos α cos k cos( k + π n α k + πn mv ob P 0 h cos α cos k n α k + π m h k E Enegy is peiodic

More information

Two Coupled Oscillators / Normal Modes

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

More information

( ) ( ) ( ) ( ) ( ) ( y )

( ) ( ) ( ) ( ) ( ) ( y ) 8. Lengh of Plne Curve The mos fmous heorem in ll of mhemics is he Pyhgoren Theorem. I s formulion s he disnce formul is used o find he lenghs of line segmens in he coordine plne. In his secion you ll

More information

Section 1.2 Angles and Angle Measure

Section 1.2 Angles and Angle Measure Sec.. ngles and ngle Measure LSSIFITION OF NGLES Secion. ngles and ngle Measure. Righ angles are angles which. Sraigh angles are angles which measure measure 90. 80. Every line forms a sraigh angle. 90

More information

Radical Expressions. Terminology: A radical will have the following; a radical sign, a radicand, and an index.

Radical Expressions. Terminology: A radical will have the following; a radical sign, a radicand, and an index. Radical Epressions Wha are Radical Epressions? A radical epression is an algebraic epression ha conains a radical. The following are eamples of radical epressions + a Terminology: A radical will have he

More information