DEDUCTION OF THE GRAVITY LAW AND QUANTUM MECHANICAL MODEL OF DISCRETIZATION IN THE MACROSCOPIC GRAVITY SYSTEM FROM SOLAR SYSTEM DATA

Size: px
Start display at page:

Download "DEDUCTION OF THE GRAVITY LAW AND QUANTUM MECHANICAL MODEL OF DISCRETIZATION IN THE MACROSCOPIC GRAVITY SYSTEM FROM SOLAR SYSTEM DATA"

Transcription

1 st Iteratioal Cogress of Serbia Society of Mechaics, 0-3 th April, 007, Kopaoik DEDUCTION OF THE GRAVITY LAW AND QUANTUM MECHANICAL MODEL OF DISCRETIZATION IN THE MACROSCOPIC GRAVITY SYSTEM FROM SOLAR SYSTEM DATA Aleksadar S. Tomić VI Gymasium, Milaa Rakića 33, 000 Belgrade Peoples observatory, Kalemegda, 000 Belgrade Abstract: The aalysis of the historical process of comig to kow the solar system from Koperik s measuremet of the plaetary distaces ad periods, ad Kepler laws of plaetary motio is applied for a recostructio of the path for a direct deductio of the law of gravity iteractio (differet from Newto s procedure) ad quatum mechaical model of the mass discretizatio i macroscopic gravity systems (Bohr-Sommerfeld s solutio), too. We used i cosideratio the ideas of Borelli, Kepler, Huiges, Boscovich, Titius ad Bode ad oe s ow cosideratio of the secod Kepler s law as a possible discrete distributio determied by atural umbers. The coclusios were: gravity costats by ature is kietic, kietic cocept demostrated the structural aalogies betwee gravity ad electrical force law with the same quatizatio rules. We extracted the possibility of uificatio of gravity ad electric force i kietic formalism. Structural aalogy of electric ad gravity iteractio, ad effors for uificatio of these physical fields, i this aalysis obtaied a importat support uificatio is possible, but o kietic level, istead used dyamic level. Key words: Newto s gravity law, Bohr s quatizatio, Solar system, epistemology, uificatio of forces. Itroductio Koperik published i the year 543 rd De revolutioibus orbium coelestium. His measuremet cofirmed cocept of world itroduced by Aristarch approximately 8 cetury ago, i which plaets revolvig aroud the Su, istead aroud the Earth. Trigoometric method has bee used by solvig the plae triagle for distace estimatio, simultaeously plaet to the Su ad plaet to the Earth. I the itervals bordered with accuracy of the measuremet Koperik obtaied permaet distaces to the Su ad very variable distaces to the Earth. With regard to the cosequeces produced o the theological doctries, usually were thought o the Koperik s astroomical revolutio [], or o the overthrow by which the Earth removed from the ceter of the world. Numerical data obtaied by Koperik presets also the same big surprise. Differece i the measured data ad adopted evaluatios util Koperik [] were remarkable. Solar system were much bigger tha it were assumed. Koperik itroduced a ew measure for distace astroomical uit, i absece of exact value for Earth s radius. Also, estimated sideral plaetary periods from itervals betwee oppositio (for exteral plaets) ad maximal elogatio (for iteral plaets), itroducig implicit a hypothesis o the summig of 63

2 A.S. Tomić: Deductio Of The Gravity Law Ad Quatum Mechaical Model Of Discretizatio From Solar System Data the agular velocities as the vector, what is the most ofte igored. As the result o this way were obtaied the possibility to calculate plaetary circular velocities, with importat detail - faster decreasig of the velocity by icreasig of the distace. Kepler held his attetio o this detail ad o the fact that seasos (determied precisely by solar positio o the celestial sphere) were ot equal i the duratio. He is lookig for cause, ito data for three decades permaetly Brahe s measuremet of plaetary positios, with the accuracy better tha each others. Result (o practically equally log calculatio) appears as Kepler s three law of plaetary motio aroud the Su, published i De harmoices mudi-liber V, 69 [3]. I Astroomia ova sive Physica coelestis [4] he proposed the mass of the celestial body as the origi of the attractio betwee celestial bodies. So were Kepler the first ma which uified celestial physics (plaetary motio) ad terrestrial physics (Galilea kietics). Both were cosidered i the frames of kietics, ad Kepler attributed to the plaets (freely movig through the space, but the most ot o the circles, ad ot uiformly) the same iertia. Lookig for explaatio appears as imperative. Galilei ad its followers regard that trasmissio of the iertia priciple to the plaets were just eough explaatio, ad igored Kepler s discovery. I these times Kepler marked ot that plaetary motio must have cetrifugal force as a compesatio i equilibrium. Borelli were the first which as scietist brig out the questio a quo movetur plaetae ad why plaets stad o these distaces.(a cetury latterly it repeat Charles Boet. [9]) He cosidered [5],[6] this problem ad gives attetio to the missed compesatio. Cosequetly followig Aristotelia method coectio of the cosequece ad cause, Borelli cocluded that i the stable circular motio must be the equilibrium. He foud geometrical explaatio for the existece of elliptical orbit (by coical sectios), cosidered problem of the stability of the Solar system as the equilibrium of the cetrifugal ad cetripetal force (usig Galilea method of reductio celestial motio o the mechaical examples from terrestrial physics of fluid ad quasi magetic iteractio). Explicit coclusio were that it what movig is iteral priciple, ot itelliget exteral while. Celestial mechaics were fouded o the priciple of coservatio the motio. Borelli had atteded that startig force i the solar system is costat. O the oscillatig pedulum he demostrated that the motio by actio of the costat cetral force at bigger distace were slowly, how it has foud Koperik for plaetary motio. Accordig to Galileo the gravity betwee plaets ad the Su were active by origi of the plaets, ad plaets followed to fall to the Su up to the momet i which achieved its actual velocities. (Freely fall to the Su is possible for quiet plaet, ad i the ay sese Galileo is right.) He cosidered i terms of his kietics oly liear gravity actio, other words make the differece betwee this ad circular motio i the cause, too. Hooke ad Newto geeralized gravity actio to all bodies i the uiverse. Method of cosideratio used by Newto is well kow, ad we wish it repeat ot. We ca ow ask the aswer to the questio: Is possible the riches of cotets i Koperik s data, Kepler s laws ad Borelli s ideas utilize, ad obtai somewhat moreover? Specially, we bare o mid explaatio o the ecessary trasit from cosequetly cotiuity to discotiuity, i cosideratio by Boscovich of stable orbit i system of few (three) body with gravity force as iteractio [7],[8], ad Titius - Bode s rule for discrete plaetary distace [9]. With a small appedix we thik that it were possible, o followig way.. Iitial data ad assumed kowledge Our cocept is very simple. I the measuremet were foud the source of motile force by Galileo i the Earth, by Koperik ad Kepler i the Su, i.e. i the material bodies. Before tha it were made Newto, Kepler brought out the hypothesis o the mass of cetral body as the cause of plaetary motio. For stable plaetary motio the ecessity of velocity ad impulse coservatio, permaet presece of the cetral force as the cause of motio, ad the equilibrium of opposite 63

3 A.S. Tomić: Deductio Of The Gravity Law Ad Quatum Mechaical Model Of Discretizatio From Solar System Data orieted forces as the coditio of the stability itroduced Borelli. Newto accepted the iertial priciple of Galileo, itroduced hypothesis of the equivalece of the gravity acceleratio o the Earth s surface ad the cetripetal acceleratio to the Moo at the smallest possible distace - the Earth s surface as the cosequece of the same origi. He defied the acceleratio as the ratio actig force /mass of exposed body ad the equilibrium of actio ad reactio implicit as vectors. O the examples of two orbital motio, first the Earth aroud the Su, ad secod the Moo aroud the Earth, supposed the same origi of attractio i both cases (or equivalet gravity costats, as alterative), usig Picard s [0] measuremet of the Earth s radius (669-67), the third Kepler s law ad defiitio of cetripetal acceleratio, Newto derived the gravity force as fuctio mass of bodies ad distace. By retroactive cosideratio obtaied also the third Kepler s law i the form which determies the sese of the Kepler s costats as the multiple of gravity costats ad the mass of cetral body - if agular velocity is used: ω r 3 = γ M. Just it is cotets hypothesis of Kepler, for which Kepler were ot have had the time to make test of statemet. How big task it were, show Newto i his Pricipia. Kepleria ad Galilea physics stay kietic, other words defied for mass uit. The coservatios laws for isolated systems were formulated latter, as a geeralizatio of Newto s mechaics Our cosideratio of the secod Kepler s law as possible discrete distributio determied by atural umber (Table ) for the ext cosideratio were eedy too. A simple procedure i coectio of these facts gave very iterestig results. 3. Deductio of quatum mechaical discretizatio We start from the third Kepler s law i the form: v r = cost, () also from the secod Kepler s law i the evidetly discrete formulatio, followig from data give i Table : vr = ( vr ). () By itroductio of fuctioal multiplier f for the velocity discrete trasformatio by distace chage, which is ukow, if Eq. divides by Eq.: v r ( vr ) ( v f) = = v = v f. vr ( vr ) (3) ad dividig Eq. by squared Eq.: v r ( vr ) ( v f) f = = = ( vr) ( v r ) r r. (4) Now isert v = v f ad r = r / f i the third Kepler s law: v r = cost = v r = ( v f) ( r ) = v r f. (5) f It is satisfied oly for: f = /, (6) i.e. velocity ad stable distace trasformatio possess the form: v = v /, r = r. (7) Direct applicatio of formulae (7) o plaets i solar system, by aalogy with atom, is ot effective for Mercury order umber = is ot adequate. But, for umbers obtaied from quatizatio of agular momet (Table) it is just adequate. 633

4 A.S. Tomić: Deductio Of The Gravity Law Ad Quatum Mechaical Model Of Discretizatio From Solar System Data km plaet r (AU) v( ) s AU km r v ( ) v km ( ) s s Pluto 39,53 4,73 86,98,9 3 0,78 30,955 Neptue 30,0 5,43 63,50 4,74 7 0,048 6,97 Ura 9,8 6,80 30,68 3, 0,458,536 Satur 9,555 9,65 9, 46,56 5 0,00 5,75 Jupiter 5,03 3,06 67,95 85,8 0,0,3 Asteroids,709 8, 49,06 63,99 8 0,086 8,086 Mars,53 4,3 36,75 9,3 6 0,058 6,069 Earth,000 9,79 9,79 443,7 5 0,089 4,96 Veus 0,73 35,0 5,3 63,0 4 0,74 4,8 Mercury 0,389 47,87 8,5 45,77 3 0,055 3,059 ** 0,655 73,, 680,58 * 0,044 46,44 6,06 07,34 Table : Quatizatio of agular momet ad eergy of mass uit i the Solar system Here we have additioal argumet. If plaetary distaces express via geometric progressio, kow as Titius-Bode rule [9] the average distace ratio of successively plaets is equal []: r / =.695 r. (8) From quatizatio of agular momet for mass uit ad third Kepler s law ca be calculated distace ad velocity of the first two (missig) plaets, as: v r = γ M = cost (9.) v = ( v r) / ( v r), r = ( v r) / v, (9.) v = ( v r) / ( v r), r = ( v r) / v. (9.3) Obtaied values are icluded i Table. It is obvious that distace ratio icreasig if plaets comig earer to the Su: r / =.695 r, r 4 / r 3 =. 859, r 3 / r =. 350, r / r = (0) Expressed with first possible plaet distace r, determied by quatizatio of agular momet, istead of real earest plaet, we have beautiful agreemet: r = r =. 999 r (.) r3 =.350 r = 9.4 r = r (.) r4 =.859 r3 = 7.9 r = r (.3) r5 = r, etc. (.4) We ca coclude that the same formulas are really valid for electrical force i the atoms ad gravitatioal force i plaetary system, with oly differece that here exist vacat positios. The formulas (7) are well kow, but here obtaied from kietic cocept, while Bohr i his atomic model derived from dyamical cocept applied to the electric force. Electrical force law, aalogous i form with gravity force law, were obtaied experimetally a cetury after appeared Pricipia. For differece related to Galileo ad Kepler which start from measured data, Bohr used much more mathematical model kow as Newto s cocept of mechaics, ad coservatio laws for system i weak iteractio with eviromet. Applyig formulae for kietic ad potetial eergy ad coservatio of eergy, valid because of big distace to earest stars, i.e. good isolatio of solar system, it ca be obtaied formula for specific eergy (eergy per mass uit) of each plaet i kietic cocept, too: E E 634

5 A.S. Tomić: Deductio Of The Gravity Law Ad Quatum Mechaical Model Of Discretizatio From Solar System Data E E = (, () m m ) ad it s obvious from last colum of Table. We obtaied formulas for velocity, distace ad eergy (pro mass uit) i kow form, but here all quatity were kietic, ot dyamic. Other words all ca stay kietic. It is origial procedure, dyamical procedure is upgraded aex. Why is it importat? Gravity quatizatio ca be realized oly i this case. For electrical quatizatio it is preferable, ot critical. It is oe from reasos why through over eight decades all attempts by uificatio of electrical ad gravity force were ot gave result. A remark. The first useful attempt of coectig formulas for electric ad gravity iteractio made Ferado Saford, just after Bohr s model were accepted []. He attempt derive Bohr s equatios from data for plaets usig oly secod ad third Kepler s law, ad foud for plaetary distaces (r) ad periods (T) relatios: r / T = Q, (3) r = Q = 0.048[ AU ], (4) startig with =3 for Mercury. This were equivalet to our formulas () ad (7) for agular momet of mass uit discrete distributio (what Saford were ot recogized), ad for distaces. For each plaet Saford lookig for formula givig eergy, but ot for mass uit. How plaetary masses were differet, obtaied result were throw of, where editor ad reviewer were ot poited out that divisio by plaetary mass make all regular, but ow as eergy of mass uit ( /T =ν frequecy, k = cost ): E / m = k ν. (5) This attempt Saford made i the best momet. But, coceptual ommissio by author ad ot eough attetio by reviewers resulted as failure. (Saford's paper author obtaied by kidess of dr Siiša Igjatović, i this momet i Toroto, Caada, after ivestigatio were fiished.) 4. Gravity law Itroduced hypothesis o the mass of cetral body as the cause of plaetary orbital motio showed as right. Oly this quatity is the same i the iteractio with each plaet. I the third Kepler's law, the costats which as multiplyer of the mass equalize quatities ad uits, is gravity costats, itroduced by liear proportioality: v r = cost = γ M. (6) Cetripetal acceleratio is equal to the ratio of squared velocity ad distace. If simple divide by r obtaies acceleratio to the cetral body: v / r = γ M / r = a c, (7) eough for descriptio of plaetary motio. Coectio of cetripetal acceleratio ad plaetary mass ito gravity force made Newto. Usig here oly Newto's the secod priciple it follows directly the gravity law: F = m ac = γ M m / r. (8) The previous cosideratio gave a possibility to defie gravity costate i solar system as Kepler's costate o mass uit of cetral body (the most correct - at miimal possible distace from the Su) as follows from Eq.: v r / M = v r / M = γ. (9) How we see, it presets also kietic quatity, ad gravity costats realy belogs to Kepler's cocept. Mass stay as a cause of motio, but determied (or harmoized) by kietic parameters. I the pairs of body Earth-Moo ad other system plaet-satelite, the same umerical value were 635

6 A.S. Tomić: Deductio Of The Gravity Law Ad Quatum Mechaical Model Of Discretizatio From Solar System Data obtaied, so that ca be word o the uiversality of this costats. Dimezioaly: 3 [ γ ] = kg s m, what ca be expressed also as claim that a multiple of mass ad squared time is iverse equivalet (o the uit circle) to the space, i.e. to volume, if the gravity costats treated as dimesioless quatity. I the same status is Coulomb's costats, defied pro uit of electricity of the cetral body. O this way it ca be word o the mass (or electricity) as origi of the space, ad the time as the measure of the chage (or evolutio) i the distributio of the mass / electricity. These categories were ot so clea defied i published papers. 5. Coclusios The historical process of how to kow the solar system from Koperik, Kepler, Huiges ad Newto is permaet preset part of scietific heritage i cotemporary educatio. With additio of Borelli idea's (ed of 6.cetury), Kepler's hypothesis o the cause of orbital motio, ad Boskovic's deductio of the trasformatio of the cotiuity ito discotiuity i gravity systems [7],[8], it appears as cosequetly logic coected with our cosideratio of the d Kepler's law as the discrete distributio determied by atural umbers - other words, with fractal structure of solar system [3]. By usig methaphysic most strog arms - logical deductio, we show that i the last etape existece of methaphysics i sciece were omited obvious possibility for short deductio of (Newto's) gravity law ad Bor- Somerfeld's solutio for discretizatio i the macroscopic gravity systems. The first atempt of coectio obtaied formulas for electrical ad gravity field, made by Saford i the year 9 were estimated as failure. Structural aalogy of electric ad gravity iteractio, ad effors for uificatio of these physical fields, i this aalysis obtaied a importat support uificatio is possible, but o cietic level, istead o used dyamic level. Refereces [] Koyre A., The astroomical revolutio, Herma (Paris) Methue (Lodo)- Corell Uiv. Press (Ithaca-NewYork), 973, [] Patricius F., Nova de uiverses philosophia / Nova sveopća folozofija, Ferrara / Zagreb, 59/97. [3] Kepler J., De harmoices mudi, Liber V, Wuetemberg, 69. [4] Kepler J., Astroomia ova sive Physica coelestis, Wuetemberg, 65. [5] Borelli J.A., Theoricae Mediceorum plaetarum ex causis physicis deductae, Flores, 666. [6] Borelli, J.A., De motioibus aturalibus a gravitate pedetibus, Bologa, 670. [7] Boskovich R., Theoria philosophiae aturalis, Veetia, Teorija prirode filozofije, Zagreb, 763/974. [8] Tomić A.S., p i Grujić P.- Ivaović M. (Eds) Epistemological problems i the sciece, (Lex uica virium i atura of Rudjer Bošković) I serbia, IKSI, Beograd, 004. [9] Tomić A., VASIONA, 4, -3, (Why plaets are where they are; I Serbia), 993. [0] Picard J., Mesure de la Terre, 67. [] Tomić A.S., Flogisto, 7, 5-68 (Plaetary distaces as the golde sectio; I Serbia), 998. [] Saford F., Popular Astroomy, 9, ( Quatum equatio i the Solar system), 9. [3] Tomić A, S., Proceed. 8 th SAUM, p. 8- Fac. Mech. Egi. Belgrade, (Fractal hierarchical structure i solar system arragemet),

ARISTOTELIAN PHYSICS

ARISTOTELIAN PHYSICS ARISTOTELIAN PHYSICS Aristoteles (Aristotle) (384-322 BC) had very strog ifluece o Europea philosophy ad sciece; everythig o Earth made of (mixture of) four elemets: earth, water, air, fire every elemet

More information

True Nature of Potential Energy of a Hydrogen Atom

True Nature of Potential Energy of a Hydrogen Atom True Nature of Potetial Eergy of a Hydroge Atom Koshu Suto Key words: Bohr Radius, Potetial Eergy, Rest Mass Eergy, Classical Electro Radius PACS codes: 365Sq, 365-w, 33+p Abstract I cosiderig the potetial

More information

Today. Homework 4 due (usual box) Center of Mass Momentum

Today. Homework 4 due (usual box) Center of Mass Momentum Today Homework 4 due (usual box) Ceter of Mass Mometum Physics 40 - L 0 slide review Coservatio of Eergy Geeralizatio of Work-Eergy Theorem Says that for ay isolated system, the total eergy is coserved

More information

Section 11.8: Power Series

Section 11.8: Power Series Sectio 11.8: Power Series 1. Power Series I this sectio, we cosider geeralizig the cocept of a series. Recall that a series is a ifiite sum of umbers a. We ca talk about whether or ot it coverges ad i

More information

Holistic Approach to the Periodic System of Elements

Holistic Approach to the Periodic System of Elements Holistic Approach to the Periodic System of Elemets N.N.Truov * D.I.Medeleyev Istitute for Metrology Russia, St.Peterburg. 190005 Moskovsky pr. 19 (Dated: February 20, 2009) Abstract: For studyig the objectivity

More information

The Mathematical Model and the Simulation Modelling Algoritm of the Multitiered Mechanical System

The Mathematical Model and the Simulation Modelling Algoritm of the Multitiered Mechanical System The Mathematical Model ad the Simulatio Modellig Algoritm of the Multitiered Mechaical System Demi Aatoliy, Kovalev Iva Dept. of Optical Digital Systems ad Techologies, The St. Petersburg Natioal Research

More information

Problem 1. Problem Engineering Dynamics Problem Set 9--Solution. Find the equation of motion for the system shown with respect to:

Problem 1. Problem Engineering Dynamics Problem Set 9--Solution. Find the equation of motion for the system shown with respect to: 2.003 Egieerig Dyamics Problem Set 9--Solutio Problem 1 Fid the equatio of motio for the system show with respect to: a) Zero sprig force positio. Draw the appropriate free body diagram. b) Static equilibrium

More information

Castiel, Supernatural, Season 6, Episode 18

Castiel, Supernatural, Season 6, Episode 18 13 Differetial Equatios the aswer to your questio ca best be epressed as a series of partial differetial equatios... Castiel, Superatural, Seaso 6, Episode 18 A differetial equatio is a mathematical equatio

More information

6.3 Testing Series With Positive Terms

6.3 Testing Series With Positive Terms 6.3. TESTING SERIES WITH POSITIVE TERMS 307 6.3 Testig Series With Positive Terms 6.3. Review of what is kow up to ow I theory, testig a series a i for covergece amouts to fidig the i= sequece of partial

More information

The Growth of Functions. Theoretical Supplement

The Growth of Functions. Theoretical Supplement The Growth of Fuctios Theoretical Supplemet The Triagle Iequality The triagle iequality is a algebraic tool that is ofte useful i maipulatig absolute values of fuctios. The triagle iequality says that

More information

) can be used instead of arbitrary distance r 0

) can be used instead of arbitrary distance r 0 Зборник на трудови од III конгрес на математичарите на Македонија Струга, Македонија, 29.IX-2.X-2005 Стр. 569-576 Proceedigs of III cogress of mathematicias of Macedoia Struga, Macedoia, 29.IX-2.X-2005

More information

Limitation of Applicability of Einstein s. Energy-Momentum Relationship

Limitation of Applicability of Einstein s. Energy-Momentum Relationship Limitatio of Applicability of Eistei s Eergy-Mometum Relatioship Koshu Suto Koshu_suto19@mbr.ifty.com Abstract Whe a particle moves through macroscopic space, for a isolated system, as its velocity icreases,

More information

3. Z Transform. Recall that the Fourier transform (FT) of a DT signal xn [ ] is ( ) [ ] = In order for the FT to exist in the finite magnitude sense,

3. Z Transform. Recall that the Fourier transform (FT) of a DT signal xn [ ] is ( ) [ ] = In order for the FT to exist in the finite magnitude sense, 3. Z Trasform Referece: Etire Chapter 3 of text. Recall that the Fourier trasform (FT) of a DT sigal x [ ] is ω ( ) [ ] X e = j jω k = xe I order for the FT to exist i the fiite magitude sese, S = x [

More information

Microscopic Theory of Transport (Fall 2003) Lecture 6 (9/19/03) Static and Short Time Properties of Time Correlation Functions

Microscopic Theory of Transport (Fall 2003) Lecture 6 (9/19/03) Static and Short Time Properties of Time Correlation Functions .03 Microscopic Theory of Trasport (Fall 003) Lecture 6 (9/9/03) Static ad Short Time Properties of Time Correlatio Fuctios Refereces -- Boo ad Yip, Chap There are a umber of properties of time correlatio

More information

A widely used display of protein shapes is based on the coordinates of the alpha carbons - - C α

A widely used display of protein shapes is based on the coordinates of the alpha carbons - - C α Nice plottig of proteis: I A widely used display of protei shapes is based o the coordiates of the alpha carbos - - C α -s. The coordiates of the C α -s are coected by a cotiuous curve that roughly follows

More information

lil fit c tai an.ie't 1111 At I 6qei ATA I Atb Y Ex Find the linear regression today power law example forhw i gl.es 6 inner product spaces

lil fit c tai an.ie't 1111 At I 6qei ATA I Atb Y Ex Find the linear regression today power law example forhw i gl.es 6 inner product spaces Math 2270-002 Week 14 otes We will ot ecessarily fiish the material from a give day's otes o that day. We may also add or subtract some material as the week progresses, but these otes represet a i-depth

More information

4.3 Growth Rates of Solutions to Recurrences

4.3 Growth Rates of Solutions to Recurrences 4.3. GROWTH RATES OF SOLUTIONS TO RECURRENCES 81 4.3 Growth Rates of Solutios to Recurreces 4.3.1 Divide ad Coquer Algorithms Oe of the most basic ad powerful algorithmic techiques is divide ad coquer.

More information

Infinite Sequences and Series

Infinite Sequences and Series Chapter 6 Ifiite Sequeces ad Series 6.1 Ifiite Sequeces 6.1.1 Elemetary Cocepts Simply speakig, a sequece is a ordered list of umbers writte: {a 1, a 2, a 3,...a, a +1,...} where the elemets a i represet

More information

The Riemann Zeta Function

The Riemann Zeta Function Physics 6A Witer 6 The Riema Zeta Fuctio I this ote, I will sketch some of the mai properties of the Riema zeta fuctio, ζ(x). For x >, we defie ζ(x) =, x >. () x = For x, this sum diverges. However, we

More information

Math 113 Exam 4 Practice

Math 113 Exam 4 Practice Math Exam 4 Practice Exam 4 will cover.-.. This sheet has three sectios. The first sectio will remid you about techiques ad formulas that you should kow. The secod gives a umber of practice questios for

More information

The Phi Power Series

The Phi Power Series The Phi Power Series I did this work i about 0 years while poderig the relatioship betwee the golde mea ad the Madelbrot set. I have fially decided to make it available from my blog at http://semresearch.wordpress.com/.

More information

Principle Of Superposition

Principle Of Superposition ecture 5: PREIMINRY CONCEP O RUCUR NYI Priciple Of uperpositio Mathematically, the priciple of superpositio is stated as ( a ) G( a ) G( ) G a a or for a liear structural system, the respose at a give

More information

Synopsis of Euler s paper. E Memoire sur la plus grande equation des planetes. (Memoir on the Maximum value of an Equation of the Planets)

Synopsis of Euler s paper. E Memoire sur la plus grande equation des planetes. (Memoir on the Maximum value of an Equation of the Planets) 1 Syopsis of Euler s paper E105 -- Memoire sur la plus grade equatio des plaetes (Memoir o the Maximum value of a Equatio of the Plaets) Compiled by Thomas J Osler ad Jase Adrew Scaramazza Mathematics

More information

7 Sequences of real numbers

7 Sequences of real numbers 40 7 Sequeces of real umbers 7. Defiitios ad examples Defiitio 7... A sequece of real umbers is a real fuctio whose domai is the set N of atural umbers. Let s : N R be a sequece. The the values of s are

More information

Chapter 4. Fourier Series

Chapter 4. Fourier Series Chapter 4. Fourier Series At this poit we are ready to ow cosider the caoical equatios. Cosider, for eample the heat equatio u t = u, < (4.) subject to u(, ) = si, u(, t) = u(, t) =. (4.) Here,

More information

DETERMINATION OF MECHANICAL PROPERTIES OF A NON- UNIFORM BEAM USING THE MEASUREMENT OF THE EXCITED LONGITUDINAL ELASTIC VIBRATIONS.

DETERMINATION OF MECHANICAL PROPERTIES OF A NON- UNIFORM BEAM USING THE MEASUREMENT OF THE EXCITED LONGITUDINAL ELASTIC VIBRATIONS. ICSV4 Cairs Australia 9- July 7 DTRMINATION OF MCHANICAL PROPRTIS OF A NON- UNIFORM BAM USING TH MASURMNT OF TH XCITD LONGITUDINAL LASTIC VIBRATIONS Pavel Aokhi ad Vladimir Gordo Departmet of the mathematics

More information

DS 100: Principles and Techniques of Data Science Date: April 13, Discussion #10

DS 100: Principles and Techniques of Data Science Date: April 13, Discussion #10 DS 00: Priciples ad Techiques of Data Sciece Date: April 3, 208 Name: Hypothesis Testig Discussio #0. Defie these terms below as they relate to hypothesis testig. a) Data Geeratio Model: Solutio: A set

More information

CHAPTER 10 INFINITE SEQUENCES AND SERIES

CHAPTER 10 INFINITE SEQUENCES AND SERIES CHAPTER 10 INFINITE SEQUENCES AND SERIES 10.1 Sequeces 10.2 Ifiite Series 10.3 The Itegral Tests 10.4 Compariso Tests 10.5 The Ratio ad Root Tests 10.6 Alteratig Series: Absolute ad Coditioal Covergece

More information

Math 155 (Lecture 3)

Math 155 (Lecture 3) Math 55 (Lecture 3) September 8, I this lecture, we ll cosider the aswer to oe of the most basic coutig problems i combiatorics Questio How may ways are there to choose a -elemet subset of the set {,,,

More information

10.6 ALTERNATING SERIES

10.6 ALTERNATING SERIES 0.6 Alteratig Series Cotemporary Calculus 0.6 ALTERNATING SERIES I the last two sectios we cosidered tests for the covergece of series whose terms were all positive. I this sectio we examie series whose

More information

Math 2784 (or 2794W) University of Connecticut

Math 2784 (or 2794W) University of Connecticut ORDERS OF GROWTH PAT SMITH Math 2784 (or 2794W) Uiversity of Coecticut Date: Mar. 2, 22. ORDERS OF GROWTH. Itroductio Gaiig a ituitive feel for the relative growth of fuctios is importat if you really

More information

f(x) dx as we do. 2x dx x also diverges. Solution: We compute 2x dx lim

f(x) dx as we do. 2x dx x also diverges. Solution: We compute 2x dx lim Math 3, Sectio 2. (25 poits) Why we defie f(x) dx as we do. (a) Show that the improper itegral diverges. Hece the improper itegral x 2 + x 2 + b also diverges. Solutio: We compute x 2 + = lim b x 2 + =

More information

Kinetics of Complex Reactions

Kinetics of Complex Reactions Kietics of Complex Reactios by Flick Colema Departmet of Chemistry Wellesley College Wellesley MA 28 wcolema@wellesley.edu Copyright Flick Colema 996. All rights reserved. You are welcome to use this documet

More information

Section 1 of Unit 03 (Pure Mathematics 3) Algebra

Section 1 of Unit 03 (Pure Mathematics 3) Algebra Sectio 1 of Uit 0 (Pure Mathematics ) Algebra Recommeded Prior Kowledge Studets should have studied the algebraic techiques i Pure Mathematics 1. Cotet This Sectio should be studied early i the course

More information

2C09 Design for seismic and climate changes

2C09 Design for seismic and climate changes 2C09 Desig for seismic ad climate chages Lecture 02: Dyamic respose of sigle-degree-of-freedom systems I Daiel Grecea, Politehica Uiversity of Timisoara 10/03/2014 Europea Erasmus Mudus Master Course Sustaiable

More information

Zeros of Polynomials

Zeros of Polynomials Math 160 www.timetodare.com 4.5 4.6 Zeros of Polyomials I these sectios we will study polyomials algebraically. Most of our work will be cocered with fidig the solutios of polyomial equatios of ay degree

More information

3.2 Properties of Division 3.3 Zeros of Polynomials 3.4 Complex and Rational Zeros of Polynomials

3.2 Properties of Division 3.3 Zeros of Polynomials 3.4 Complex and Rational Zeros of Polynomials Math 60 www.timetodare.com 3. Properties of Divisio 3.3 Zeros of Polyomials 3.4 Complex ad Ratioal Zeros of Polyomials I these sectios we will study polyomials algebraically. Most of our work will be cocered

More information

PHYS-3301 Lecture 7. CHAPTER 4 Structure of the Atom. Rutherford Scattering. Sep. 18, 2018

PHYS-3301 Lecture 7. CHAPTER 4 Structure of the Atom. Rutherford Scattering. Sep. 18, 2018 CHAPTER 4 Structure of the Atom PHYS-3301 Lecture 7 4.1 The Atomic Models of Thomso ad Rutherford 4.2 Rutherford Scatterig 4.3 The Classic Atomic Model 4.4 The Bohr Model of the Hydroge Atom 4.5 Successes

More information

Section 1.1. Calculus: Areas And Tangents. Difference Equations to Differential Equations

Section 1.1. Calculus: Areas And Tangents. Difference Equations to Differential Equations Differece Equatios to Differetial Equatios Sectio. Calculus: Areas Ad Tagets The study of calculus begis with questios about chage. What happes to the velocity of a swigig pedulum as its positio chages?

More information

EXPERIMENT OF SIMPLE VIBRATION

EXPERIMENT OF SIMPLE VIBRATION EXPERIMENT OF SIMPLE VIBRATION. PURPOSE The purpose of the experimet is to show free vibratio ad damped vibratio o a system havig oe degree of freedom ad to ivestigate the relatioship betwee the basic

More information

MAT1026 Calculus II Basic Convergence Tests for Series

MAT1026 Calculus II Basic Convergence Tests for Series MAT026 Calculus II Basic Covergece Tests for Series Egi MERMUT 202.03.08 Dokuz Eylül Uiversity Faculty of Sciece Departmet of Mathematics İzmir/TURKEY Cotets Mootoe Covergece Theorem 2 2 Series of Real

More information

Mechatronics. Time Response & Frequency Response 2 nd -Order Dynamic System 2-Pole, Low-Pass, Active Filter

Mechatronics. Time Response & Frequency Response 2 nd -Order Dynamic System 2-Pole, Low-Pass, Active Filter Time Respose & Frequecy Respose d -Order Dyamic System -Pole, Low-Pass, Active Filter R 4 R 7 C 5 e i R 1 C R 3 - + R 6 - + e out Assigmet: Perform a Complete Dyamic System Ivestigatio of the Two-Pole,

More information

Two or more points can be used to describe a rigid body. This will eliminate the need to define rotational coordinates for the body!

Two or more points can be used to describe a rigid body. This will eliminate the need to define rotational coordinates for the body! OINTCOORDINATE FORMULATION Two or more poits ca be used to describe a rigid body. This will elimiate the eed to defie rotatioal coordiates for the body i z r i i, j r j j rimary oits: The coordiates of

More information

SEQUENCES AND SERIES

SEQUENCES AND SERIES Sequeces ad 6 Sequeces Ad SEQUENCES AND SERIES Successio of umbers of which oe umber is desigated as the first, other as the secod, aother as the third ad so o gives rise to what is called a sequece. Sequeces

More information

The Random Walk For Dummies

The Random Walk For Dummies The Radom Walk For Dummies Richard A Mote Abstract We look at the priciples goverig the oe-dimesioal discrete radom walk First we review five basic cocepts of probability theory The we cosider the Beroulli

More information

MID-YEAR EXAMINATION 2018 H2 MATHEMATICS 9758/01. Paper 1 JUNE 2018

MID-YEAR EXAMINATION 2018 H2 MATHEMATICS 9758/01. Paper 1 JUNE 2018 MID-YEAR EXAMINATION 08 H MATHEMATICS 9758/0 Paper JUNE 08 Additioal Materials: Writig Paper, MF6 Duratio: hours DO NOT OPEN THIS BOOKLET UNTIL YOU ARE TOLD TO DO SO READ THESE INSTRUCTIONS FIRST Write

More information

Position Time Graphs 12.1

Position Time Graphs 12.1 12.1 Positio Time Graphs Figure 3 Motio with fairly costat speed Chapter 12 Distace (m) A Crae Flyig Figure 1 Distace time graph showig motio with costat speed A Crae Flyig Positio (m [E] of pod) We kow

More information

The standard deviation of the mean

The standard deviation of the mean Physics 6C Fall 20 The stadard deviatio of the mea These otes provide some clarificatio o the distictio betwee the stadard deviatio ad the stadard deviatio of the mea.. The sample mea ad variace Cosider

More information

17 Phonons and conduction electrons in solids (Hiroshi Matsuoka)

17 Phonons and conduction electrons in solids (Hiroshi Matsuoka) 7 Phoos ad coductio electros i solids Hiroshi Matsuoa I this chapter we will discuss a miimal microscopic model for phoos i a solid ad a miimal microscopic model for coductio electros i a simple metal.

More information

ANALYSIS OF EXPERIMENTAL ERRORS

ANALYSIS OF EXPERIMENTAL ERRORS ANALYSIS OF EXPERIMENTAL ERRORS All physical measuremets ecoutered i the verificatio of physics theories ad cocepts are subject to ucertaities that deped o the measurig istrumets used ad the coditios uder

More information

Lesson 10: Limits and Continuity

Lesson 10: Limits and Continuity www.scimsacademy.com Lesso 10: Limits ad Cotiuity SCIMS Academy 1 Limit of a fuctio The cocept of limit of a fuctio is cetral to all other cocepts i calculus (like cotiuity, derivative, defiite itegrals

More information

Similarity Solutions to Unsteady Pseudoplastic. Flow Near a Moving Wall

Similarity Solutions to Unsteady Pseudoplastic. Flow Near a Moving Wall Iteratioal Mathematical Forum, Vol. 9, 04, o. 3, 465-475 HIKARI Ltd, www.m-hikari.com http://dx.doi.org/0.988/imf.04.48 Similarity Solutios to Usteady Pseudoplastic Flow Near a Movig Wall W. Robi Egieerig

More information

MAT 271 Project: Partial Fractions for certain rational functions

MAT 271 Project: Partial Fractions for certain rational functions MAT 7 Project: Partial Fractios for certai ratioal fuctios Prerequisite kowledge: partial fractios from MAT 7, a very good commad of factorig ad complex umbers from Precalculus. To complete this project,

More information

Number of fatalities X Sunday 4 Monday 6 Tuesday 2 Wednesday 0 Thursday 3 Friday 5 Saturday 8 Total 28. Day

Number of fatalities X Sunday 4 Monday 6 Tuesday 2 Wednesday 0 Thursday 3 Friday 5 Saturday 8 Total 28. Day LECTURE # 8 Mea Deviatio, Stadard Deviatio ad Variace & Coefficiet of variatio Mea Deviatio Stadard Deviatio ad Variace Coefficiet of variatio First, we will discuss it for the case of raw data, ad the

More information

Physics 232 Gauge invariance of the magnetic susceptibilty

Physics 232 Gauge invariance of the magnetic susceptibilty Physics 232 Gauge ivariace of the magetic susceptibilty Peter Youg (Dated: Jauary 16, 2006) I. INTRODUCTION We have see i class that the followig additioal terms appear i the Hamiltoia o addig a magetic

More information

Relations between the continuous and the discrete Lotka power function

Relations between the continuous and the discrete Lotka power function Relatios betwee the cotiuous ad the discrete Lotka power fuctio by L. Egghe Limburgs Uiversitair Cetrum (LUC), Uiversitaire Campus, B-3590 Diepebeek, Belgium ad Uiversiteit Atwerpe (UA), Campus Drie Eike,

More information

Sequences, Mathematical Induction, and Recursion. CSE 2353 Discrete Computational Structures Spring 2018

Sequences, Mathematical Induction, and Recursion. CSE 2353 Discrete Computational Structures Spring 2018 CSE 353 Discrete Computatioal Structures Sprig 08 Sequeces, Mathematical Iductio, ad Recursio (Chapter 5, Epp) Note: some course slides adopted from publisher-provided material Overview May mathematical

More information

CALCULATION OF FIBONACCI VECTORS

CALCULATION OF FIBONACCI VECTORS CALCULATION OF FIBONACCI VECTORS Stuart D. Aderso Departmet of Physics, Ithaca College 953 Daby Road, Ithaca NY 14850, USA email: saderso@ithaca.edu ad Dai Novak Departmet of Mathematics, Ithaca College

More information

Recurrence Relations

Recurrence Relations Recurrece Relatios Aalysis of recursive algorithms, such as: it factorial (it ) { if (==0) retur ; else retur ( * factorial(-)); } Let t be the umber of multiplicatios eeded to calculate factorial(). The

More information

Chapter 6 Infinite Series

Chapter 6 Infinite Series Chapter 6 Ifiite Series I the previous chapter we cosidered itegrals which were improper i the sese that the iterval of itegratio was ubouded. I this chapter we are goig to discuss a topic which is somewhat

More information

An Introduction to Randomized Algorithms

An Introduction to Randomized Algorithms A Itroductio to Radomized Algorithms The focus of this lecture is to study a radomized algorithm for quick sort, aalyze it usig probabilistic recurrece relatios, ad also provide more geeral tools for aalysis

More information

Gravity An Introduction

Gravity An Introduction Gravity A Itroductio Reier Rummel Istitute of Advaced Study (IAS) Techische Uiversität Müche Lecture Oe 5th ESA Earth Observatio Summer School 2-13 August 2010, ESA-ESRIN, Frascati / Italy gravitatio ad

More information

mx bx kx F t. dt IR I LI V t, Q LQ RQ V t,

mx bx kx F t. dt IR I LI V t, Q LQ RQ V t, Lecture 5 omplex Variables II (Applicatios i Physics) (See hapter i Boas) To see why complex variables are so useful cosider first the (liear) mechaics of a sigle particle described by Newto s equatio

More information

Math 113 Exam 3 Practice

Math 113 Exam 3 Practice Math Exam Practice Exam will cover.-.9. This sheet has three sectios. The first sectio will remid you about techiques ad formulas that you should kow. The secod gives a umber of practice questios for you

More information

Structural Functionality as a Fundamental Property of Boolean Algebra and Base for Its Real-Valued Realizations

Structural Functionality as a Fundamental Property of Boolean Algebra and Base for Its Real-Valued Realizations Structural Fuctioality as a Fudametal Property of Boolea Algebra ad Base for Its Real-Valued Realizatios Draga G. Radojević Uiversity of Belgrade, Istitute Mihajlo Pupi, Belgrade draga.radojevic@pupi.rs

More information

ECON 3150/4150, Spring term Lecture 3

ECON 3150/4150, Spring term Lecture 3 Itroductio Fidig the best fit by regressio Residuals ad R-sq Regressio ad causality Summary ad ext step ECON 3150/4150, Sprig term 2014. Lecture 3 Ragar Nymoe Uiversity of Oslo 21 Jauary 2014 1 / 30 Itroductio

More information

CALCULUS BASIC SUMMER REVIEW

CALCULUS BASIC SUMMER REVIEW CALCULUS BASIC SUMMER REVIEW NAME rise y y y Slope of a o vertical lie: m ru Poit Slope Equatio: y y m( ) The slope is m ad a poit o your lie is, ). ( y Slope-Itercept Equatio: y m b slope= m y-itercept=

More information

x a x a Lecture 2 Series (See Chapter 1 in Boas)

x a x a Lecture 2 Series (See Chapter 1 in Boas) Lecture Series (See Chapter i Boas) A basic ad very powerful (if pedestria, recall we are lazy AD smart) way to solve ay differetial (or itegral) equatio is via a series expasio of the correspodig solutio

More information

Minimal surface area position of a convex body is not always an M-position

Minimal surface area position of a convex body is not always an M-position Miimal surface area positio of a covex body is ot always a M-positio Christos Saroglou Abstract Milma proved that there exists a absolute costat C > 0 such that, for every covex body i R there exists a

More information

The Wave Function and Quantum Reality

The Wave Function and Quantum Reality The Wave Fuctio ad Quatum Reality Sha Gao Uit for History ad Philosophy of Sciece & Cetre for Time, SOPHI Uiversity of Sydey, Sydey, NSW 006, Australia Abstract. We ivestigate the meaig of the wave fuctio

More information

The Pendulum. Purpose

The Pendulum. Purpose The Pedulum Purpose To carry out a example illustratig how physics approaches ad solves problems. The example used here is to explore the differet factors that determie the period of motio of a pedulum.

More information

Fall 2013 MTH431/531 Real analysis Section Notes

Fall 2013 MTH431/531 Real analysis Section Notes Fall 013 MTH431/531 Real aalysis Sectio 8.1-8. Notes Yi Su 013.11.1 1. Defiitio of uiform covergece. We look at a sequece of fuctios f (x) ad study the coverget property. Notice we have two parameters

More information

Similarity between quantum mechanics and thermodynamics: Entropy, temperature, and Carnot cycle

Similarity between quantum mechanics and thermodynamics: Entropy, temperature, and Carnot cycle Similarity betwee quatum mechaics ad thermodyamics: Etropy, temperature, ad Carot cycle Sumiyoshi Abe 1,,3 ad Shiji Okuyama 1 1 Departmet of Physical Egieerig, Mie Uiversity, Mie 514-8507, Japa Istitut

More information

The "Last Riddle" of Pierre de Fermat, II

The Last Riddle of Pierre de Fermat, II The "Last Riddle" of Pierre de Fermat, II Alexader Mitkovsky mitkovskiy@gmail.com Some time ago, I published a work etitled, "The Last Riddle" of Pierre de Fermat " i which I had writte a proof of the

More information

Stopping oscillations of a simple harmonic oscillator using an impulse force

Stopping oscillations of a simple harmonic oscillator using an impulse force It. J. Adv. Appl. Math. ad Mech. 5() (207) 6 (ISSN: 2347-2529) IJAAMM Joural homepage: www.ijaamm.com Iteratioal Joural of Advaces i Applied Mathematics ad Mechaics Stoppig oscillatios of a simple harmoic

More information

Discrete Mathematics for CS Spring 2008 David Wagner Note 22

Discrete Mathematics for CS Spring 2008 David Wagner Note 22 CS 70 Discrete Mathematics for CS Sprig 2008 David Wager Note 22 I.I.D. Radom Variables Estimatig the bias of a coi Questio: We wat to estimate the proportio p of Democrats i the US populatio, by takig

More information

Hydrogen (atoms, molecules) in external fields. Static electric and magnetic fields Oscyllating electromagnetic fields

Hydrogen (atoms, molecules) in external fields. Static electric and magnetic fields Oscyllating electromagnetic fields Hydroge (atoms, molecules) i exteral fields Static electric ad magetic fields Oscyllatig electromagetic fields Everythig said up to ow has to be modified more or less strogly if we cosider atoms (ad ios)

More information

Statistics 511 Additional Materials

Statistics 511 Additional Materials Cofidece Itervals o mu Statistics 511 Additioal Materials This topic officially moves us from probability to statistics. We begi to discuss makig ifereces about the populatio. Oe way to differetiate probability

More information

POWER SERIES SOLUTION OF FIRST ORDER MATRIX DIFFERENTIAL EQUATIONS

POWER SERIES SOLUTION OF FIRST ORDER MATRIX DIFFERENTIAL EQUATIONS Joural of Applied Mathematics ad Computatioal Mechaics 4 3(3) 3-8 POWER SERIES SOLUION OF FIRS ORDER MARIX DIFFERENIAL EQUAIONS Staisław Kukla Izabela Zamorska Istitute of Mathematics Czestochowa Uiversity

More information

EE / EEE SAMPLE STUDY MATERIAL. GATE, IES & PSUs Signal System. Electrical Engineering. Postal Correspondence Course

EE / EEE SAMPLE STUDY MATERIAL. GATE, IES & PSUs Signal System. Electrical Engineering. Postal Correspondence Course Sigal-EE Postal Correspodece Course 1 SAMPLE STUDY MATERIAL Electrical Egieerig EE / EEE Postal Correspodece Course GATE, IES & PSUs Sigal System Sigal-EE Postal Correspodece Course CONTENTS 1. SIGNAL

More information

Boundary layer problem on conveyor belt. Gabriella Bognár University of Miskolc 3515 Miskolc-Egyetemváros, Hungary

Boundary layer problem on conveyor belt. Gabriella Bognár University of Miskolc 3515 Miskolc-Egyetemváros, Hungary Boudary layer problem o coveyor belt Gabriella Bogár Uiversity of Miskolc 355 Miskolc-Egyetemváros, Hugary e-mail: matvbg@ui-miskolc.hu Abstract: A techologically importat source of the boudary layer pheomeo

More information

CHAPTER 8 SYSTEMS OF PARTICLES

CHAPTER 8 SYSTEMS OF PARTICLES CHAPTER 8 SYSTES OF PARTICLES CHAPTER 8 COLLISIONS 45 8. CENTER OF ASS The ceter of mass of a system of particles or a rigid body is the poit at which all of the mass are cosidered to be cocetrated there

More information

1 Adiabatic and diabatic representations

1 Adiabatic and diabatic representations 1 Adiabatic ad diabatic represetatios 1.1 Bor-Oppeheimer approximatio The time-idepedet Schrödiger equatio for both electroic ad uclear degrees of freedom is Ĥ Ψ(r, R) = E Ψ(r, R), (1) where the full molecular

More information

The z-transform. 7.1 Introduction. 7.2 The z-transform Derivation of the z-transform: x[n] = z n LTI system, h[n] z = re j

The z-transform. 7.1 Introduction. 7.2 The z-transform Derivation of the z-transform: x[n] = z n LTI system, h[n] z = re j The -Trasform 7. Itroductio Geeralie the complex siusoidal represetatio offered by DTFT to a represetatio of complex expoetial sigals. Obtai more geeral characteristics for discrete-time LTI systems. 7.

More information

Physics 324, Fall Dirac Notation. These notes were produced by David Kaplan for Phys. 324 in Autumn 2001.

Physics 324, Fall Dirac Notation. These notes were produced by David Kaplan for Phys. 324 in Autumn 2001. Physics 324, Fall 2002 Dirac Notatio These otes were produced by David Kapla for Phys. 324 i Autum 2001. 1 Vectors 1.1 Ier product Recall from liear algebra: we ca represet a vector V as a colum vector;

More information

WHAT IS THE PROBABILITY FUNCTION FOR LARGE TSUNAMI WAVES? ABSTRACT

WHAT IS THE PROBABILITY FUNCTION FOR LARGE TSUNAMI WAVES? ABSTRACT WHAT IS THE PROBABILITY FUNCTION FOR LARGE TSUNAMI WAVES? Harold G. Loomis Hoolulu, HI ABSTRACT Most coastal locatios have few if ay records of tsuami wave heights obtaied over various time periods. Still

More information

GUIDELINES ON REPRESENTATIVE SAMPLING

GUIDELINES ON REPRESENTATIVE SAMPLING DRUGS WORKING GROUP VALIDATION OF THE GUIDELINES ON REPRESENTATIVE SAMPLING DOCUMENT TYPE : REF. CODE: ISSUE NO: ISSUE DATE: VALIDATION REPORT DWG-SGL-001 002 08 DECEMBER 2012 Ref code: DWG-SGL-001 Issue

More information

ABOUT CHAOS AND SENSITIVITY IN TOPOLOGICAL DYNAMICS

ABOUT CHAOS AND SENSITIVITY IN TOPOLOGICAL DYNAMICS ABOUT CHAOS AND SENSITIVITY IN TOPOLOGICAL DYNAMICS EDUARD KONTOROVICH Abstract. I this work we uify ad geeralize some results about chaos ad sesitivity. Date: March 1, 005. 1 1. Symbolic Dyamics Defiitio

More information

PHYS-3301 Lecture 10. Wave Packet Envelope Wave Properties of Matter and Quantum Mechanics I CHAPTER 5. Announcement. Sep.

PHYS-3301 Lecture 10. Wave Packet Envelope Wave Properties of Matter and Quantum Mechanics I CHAPTER 5. Announcement. Sep. Aoucemet Course webpage http://www.phys.ttu.edu/~slee/3301/ PHYS-3301 Lecture 10 HW3 (due 10/4) Chapter 5 4, 8, 11, 15, 22, 27, 36, 40, 42 Sep. 27, 2018 Exam 1 (10/4) Chapters 3, 4, & 5 CHAPTER 5 Wave

More information

September 2012 C1 Note. C1 Notes (Edexcel) Copyright - For AS, A2 notes and IGCSE / GCSE worksheets 1

September 2012 C1 Note. C1 Notes (Edexcel) Copyright   - For AS, A2 notes and IGCSE / GCSE worksheets 1 September 0 s (Edecel) Copyright www.pgmaths.co.uk - For AS, A otes ad IGCSE / GCSE worksheets September 0 Copyright www.pgmaths.co.uk - For AS, A otes ad IGCSE / GCSE worksheets September 0 Copyright

More information

( ) ( ), (S3) ( ). (S4)

( ) ( ), (S3) ( ). (S4) Ultrasesitivity i phosphorylatio-dephosphorylatio cycles with little substrate: Supportig Iformatio Bruo M.C. Martis, eter S. Swai 1. Derivatio of the equatios associated with the mai model From the differetial

More information

SPEC/4/PHYSI/SPM/ENG/TZ0/XX PHYSICS PAPER 1 SPECIMEN PAPER. 45 minutes INSTRUCTIONS TO CANDIDATES

SPEC/4/PHYSI/SPM/ENG/TZ0/XX PHYSICS PAPER 1 SPECIMEN PAPER. 45 minutes INSTRUCTIONS TO CANDIDATES SPEC/4/PHYSI/SPM/ENG/TZ0/XX PHYSICS STANDARD LEVEL PAPER 1 SPECIMEN PAPER 45 miutes INSTRUCTIONS TO CANDIDATES Do ot ope this examiatio paper util istructed to do so. Aswer all the questios. For each questio,

More information

EDEXCEL NATIONAL CERTIFICATE UNIT 4 MATHEMATICS FOR TECHNICIANS OUTCOME 4 - CALCULUS

EDEXCEL NATIONAL CERTIFICATE UNIT 4 MATHEMATICS FOR TECHNICIANS OUTCOME 4 - CALCULUS EDEXCEL NATIONAL CERTIFICATE UNIT 4 MATHEMATICS FOR TECHNICIANS OUTCOME 4 - CALCULUS TUTORIAL 1 - DIFFERENTIATION Use the elemetary rules of calculus arithmetic to solve problems that ivolve differetiatio

More information

1 Inferential Methods for Correlation and Regression Analysis

1 Inferential Methods for Correlation and Regression Analysis 1 Iferetial Methods for Correlatio ad Regressio Aalysis I the chapter o Correlatio ad Regressio Aalysis tools for describig bivariate cotiuous data were itroduced. The sample Pearso Correlatio Coefficiet

More information

A PROOF OF THE TWIN PRIME CONJECTURE AND OTHER POSSIBLE APPLICATIONS

A PROOF OF THE TWIN PRIME CONJECTURE AND OTHER POSSIBLE APPLICATIONS A PROOF OF THE TWI PRIME COJECTURE AD OTHER POSSIBLE APPLICATIOS by PAUL S. BRUCKMA 38 Frot Street, #3 aaimo, BC V9R B8 (Caada) e-mail : pbruckma@hotmail.com ABSTRACT : A elemetary proof of the Twi Prime

More information

Time-Domain Representations of LTI Systems

Time-Domain Representations of LTI Systems 2.1 Itroductio Objectives: 1. Impulse resposes of LTI systems 2. Liear costat-coefficiets differetial or differece equatios of LTI systems 3. Bloc diagram represetatios of LTI systems 4. State-variable

More information

Probability, Expectation Value and Uncertainty

Probability, Expectation Value and Uncertainty Chapter 1 Probability, Expectatio Value ad Ucertaity We have see that the physically observable properties of a quatum system are represeted by Hermitea operators (also referred to as observables ) such

More information

The Logical Analysis of the Special Theory of Relativity: Lesson for Nobel Laureate in Physics

The Logical Analysis of the Special Theory of Relativity: Lesson for Nobel Laureate in Physics The Logical Aalysis of the Special Theory of Relativity: Lesso for Nobel Laureate i Physics Temur Z. Kalaov Home of Physical Problems, Pisatelskaya 6a, 7 Tashket, Uzbekista tzk_uz@yahoo.com, t.z.kalaov@mail.ru,

More information

Several properties of new ellipsoids

Several properties of new ellipsoids Appl. Math. Mech. -Egl. Ed. 008 9(7):967 973 DOI 10.1007/s10483-008-0716-y c Shaghai Uiversity ad Spriger-Verlag 008 Applied Mathematics ad Mechaics (Eglish Editio) Several properties of ew ellipsoids

More information

A NEW CLASS OF 2-STEP RATIONAL MULTISTEP METHODS

A NEW CLASS OF 2-STEP RATIONAL MULTISTEP METHODS Jural Karya Asli Loreka Ahli Matematik Vol. No. (010) page 6-9. Jural Karya Asli Loreka Ahli Matematik A NEW CLASS OF -STEP RATIONAL MULTISTEP METHODS 1 Nazeeruddi Yaacob Teh Yua Yig Norma Alias 1 Departmet

More information