NEWTON'S SECOND LAW AND CURVILINEAR MOTION OF A MATERIAL PARTICLE. Yuriy Zhivotov Yuzhnoye State Design Office, Dniepropetrovsk, Ukraine

Size: px
Start display at page:

Download "NEWTON'S SECOND LAW AND CURVILINEAR MOTION OF A MATERIAL PARTICLE. Yuriy Zhivotov Yuzhnoye State Design Office, Dniepropetrovsk, Ukraine"

Transcription

1 NEWTON'S SECOND LAW AND CURVILINEAR MOTION OF A MATERIAL PARTICLE Yuriy Zhivotov Yuzhoye State Desig Office, Diepropetrovsk, Ukraie Summary The Newto's secod law is cosidered with referece to motio of a material particle alog a curviliear trajectory. It is show that a chage i mometum of a material particle creates a tagetial ad cetripetal force. The equatios of motio of a particle were obtaied. It is show that motio of a particle requires applicatio of a mometum force at presece of a reactio force. It is show that a work of a tagetial ad cetripetal force chages the magitude ad directio of a kietic eergy vector. Newto gave the followig defiitio of the secod law of motio with referece to the rectiliear motio of a material particle with a mass ad acceleratio d mv is i proportio to the applied m a : Chage of mometum ( ) mometum force F ad takes place i the lie of the straight lie alog which this force acts. F = ma = d ( mv ) / dt () This law provides for a chage i mometum of the material particle without a chage i the directio of its motio. However, while a free material particle moves alog a curviliear trajectory, the mometum magitude ad directio may vary []. Let us assume that the material particle moves alog a covex curviliear trajectory from left to right, the directio of the velocity chagig clockwise. Let us assume that withi a short period of time t t 0 the mometum of the material particle mv 0 has icreased ad is equal to mv, a small agle ϕ havig bee formed betwee the directio of the mometum vector mv ad the directio of the mometum vector mv 0 (Figure ). Figure Let us itroduce a additioal mometum vector mv 0 so that a magitude of the mometum vector mv0 + mv is equal to that of the mometum vector 0 mv. Let us joi the termius of the additioal vector mv 0 ad the termius of the vector mv ad we shall obtai a vector mv 02. Therefore, we ca write dow the followig vector equatio i view of the small agle ϕ = siϕ ad si 0 = 0 Proceedig to the limit, if t t, we shall obtai ( ) 0 0 mv mv0 = mv0 + mv02 (2) d( mv)/ dt = ma + ma = F + F (3) where ma = mv siϕ si 0 / dt = mvϕ/ dt = mvw, ω is the agular velocity, F is the tagetial force taget to the curviliear trajectory, F is the cetripetal force with the directio perpedicular to the force F. I this defiitio of the forces brigig about the chage i mometum of the material particle, the directio of the force F coicides with that of the vector a, ad the directio of the force F, with that of the vector a. The equatio of a accelerated motio of the free material particle alog the curviliear trajectory is as follows: F + F = ma + ma (4) For the purpose of cosideratio, we selected a covex trajectory of the material particle motio. If we assume that the covex trajectory gradually turs ito a cocave trajectory, the the chage of the velocity directio will happe aticlockwise. The positio of the istataeous radius of rotatio will chage cosetaeously. The equatios

2 (2), (3) ad (4) will ot chage. If mechaical costraits impose requiremets of kiematical or geometric ature, the the chage of mometum of the material particle should be writte as follows where ( ) / d mv dt = F + R (5) R is the costrait reactio force that requires a additioal tagetial force for ow creatio. I this case, the motio equatio for a costraied particle will be as follows F = ma + ma (6) Let us cosider some features of the equatio (4). If F = 0, the ma = 0. If F is the gravitatio force, the from the equatio (4) we shall obtai a certai equatio of motio of the satellite i circular orbit. The force F esures the material poit motio roud a circle. This force is ot a mometum force. I this case we obtai that F should be equal to ma + ma. If we additioally assume tha the acceleratio a ca be equal to zero, we shall obtai that F = mvω. It results from this that at presece of costraits a uiform motio of the material particle roud a circle requires applicatio of a tagetial force. It is also worthwhile otig that the defiitio of the forces (3) brigig about the chage i mometum of the material particle alog the curviliear trajectory does ot have a effect o the defiitio of the chage i a momet of mometum relatively to the istataeous ceter of rotatio. The chage of the momet of mometum of the material particle relatively to the istataeous ceter of rotatio has its usual view: ( ) ( ) dmomv [ ]/ dt= Mo F (7) This is explaied by the fact that the directio of vector F passes through a poit relatively to which the momet is defied, ad the momet from the force F is therefore equal to zero. The equatio (3) allows a trasitio to the otio of a kietic eergy ad a work of forces. Let us assume that i a time t the material particle moved from the poit M A to the poit M B of the trajectory. Let us break the traslatio s ito sectors s. Let us multiply the right ad left parts of the equatio (3) by the mea velocity s / t (a scalar). This operatio does ot chage the magitudes or directios of the vectors i the equatio (3). As a result, we obtai the followig vector equatio: or where 2 F s = mv ϕ s s s d( mv) = ma dt+ ma dt (8) t t t mv v /2 mv v /2= F s + F s (9) 0 0 I view of the traslatio s of the material particle from the poit M A to the poit M B withi the time t, we obtai mv ( ) v ( ) /2 mv ( ) v ( ) /2 = A M M M M ( M M ) + A ( MA MB),, B B A A A B (0) The equatio (0) shows that the chage of the magitude ad directio of kietic eergy is accomplished by the work of force for traslatio ad the work of force for chagig the kietic eergy vector directio. Here, the work of force is a scalar. CONCLUSIONS The obtaied research results allow obtaiig differetial equatios of motio ad solvig problems of traslatory motio of a material particle ad a body alog a curviliear trajectory. Refereces [] Тарг С.М.: Краткий курс теоретической механики. Москва. Высшая школа стр. /Targ S.M. Cocise Course i Classical Mechaics, Moscow, Vysshaya Shkola, 966, 46 p./ Cotiuatio o the followig page!

3 AUGUST 24 30, 2008 Dr Yuriy Zhivotov Mechaics 3, Krivorozhskaya Street, Diepropetrovsk 49008, UKRAINE Diepropetrovsk Depropetrovsk regio, Ukraie Adelaide, April 22, 2008 PROFESSOR ERNIE TUCK PRESIDENT, ICTAM2008 LEVEL 4, 0 PULTENEY STREET THE UNIVERSITY OF ADELAIDE SA 5005 AUSTRALIA Dear Dr Zhivotov, I am writig o behalf of the Cogress Committee of lutam with referece to your paper with ICTAM etitled NEWTON'S SECOND LAW AND CURVILINEAR MOTION OF A MATERIAL PARTICLE submitted to the 22 d Iteratioal Cogress of Theoretical ad Applied Mechaics (ICTAM2008). Ufortuately the umber of papers submitted greatly exceeded the umber that could be accommodated i the program ad I regret to iform you that we could ot accept your paper for presetatio. I hope you will, evertheless, be able to participate i the Cogress, whose success depeds o those who atted the lectures ad participate i discussios as much as o those who make the formal presetatios. Complete details about the Cogress, icludig registratio, may be foud o the web site The orgaizers joi me i expressig their hope that you will participate i this importat mechaics evet. A formal ivitatio to atted ICTAM2008 follows. I look forward to seeig you i Adelaide. With best wishes, Yours sicerely Timothy J. Pedley Secretary, Cogress Committee of IUTAM Zhivotov s aswer! (O 2/05/2008, at 9:20 PM) ICTAM 2008, Presidet Professor Erie Tuck, The Uiversity of Adelaide. eotuck@iterode.o.et Dear Professor Erie Tuck. I have prepared a paper «NEWTON'S SECOND LAW AND CURVILINEAR TRANSLATIONAL MOTION OF THE BODY» (idetificatio umber 03) for participatio i the XXII Iteratioal Cogress of Theoretical ad Applied Mechaics, to be held i Adelaide, Australia betwee August I a paper it is show, that: I a paper it is show, that:

4 - the moder formulatio of the Newto's secod law is erroeous: the formulatio of the law substitutes idea of Lagrage to express ay force through force of iertia. The ote: The moder formulatio of the secod law substitutes the formulatio of the Newto's third law; - chage of quatity of movemet of a body ca occur both o magitude, ad o a directio. Thus forces should make work for chage of quatity of movemet of a body o magitude ad a directio; - chage of quatity of movemet demads the appedix to a body of two mutually perpedicular forces: drivig force ad cetripetal force. Cetripetal force very much frequetly is abset i egieerig practice. I this case drivig force should compesate absece of cetripetal force. I.e. i mechaisms cetripetal forces are created due to work of drivig forces; - eve uiform movemet of a material poit cocerig the ceter of rotatio demads the appedix of drivig force which makes work o chage of a directio of its movemet. Hece, uiform rotatio of a material poit o a circle demads expeses of eergy; - the existig mechaics is ot suitable for the descriptio of curviliear movemet of a body ad the decisio of this problem is resulted. The give paper is the basic documet, which advaces ew ideas i theoretical mechaics. These ideas will result i radical processig mechaics. Orgaizers of the cogress have set the followig message: I am writig o behalf of the Cogress Committee of lutam with referece to your paper with ICTAM etitled NEWTON'S SECOND LAW AND CURVILINEAR MOTION OF A MATERIAL PARTICLE submitted to the 22d Iteratioal Cogress of Theoretical ad Applied Mechaics (ICTAM2008). Ufortuately the umber of papers submitted greatly exceeded the umber that could be accommodated i the program ad I regret to iform you that we could ot accept your paper for presetatio. However orgaizers of the cogress have ot set commets of reviewers o a paper. Absece the commet does ot allow to reveal a mistake of reviewers ad to exclude artificial obstacles for promotio of ew ideas i mechaics. I this coectio, I ask you to direct to my address of commets of reviewers. Best regards, Yu. Zhivotov The aswer to the Zhivotov's letter! (O AM 8:08:27) Dear Professor Zhivotov, Thak you for your . Ufortuately the umber of papers submitted greatly exceeded the umber that could be accommodated i the program ad we regret to iform you that we caot accept your paper for presetatio.

5 We hope you will, evertheless, be able to participate i the Cogress, whose success depeds o those who atted the lectures ad participate i discussios as much as o those who make the formal presetatios. To participate i this importat mechaics evet please go to our registratio page. Best regards Jim Deier Associate Professor Jim Deier Secretary Geeral ICTAM2008 School of Mathematical Scieces The Uiversity of Adelaide South Australia 5005 Australia Phoe: (+68) Zhivotov s aswer! (Date: ) ICTAM 2008, Presidet Professor Erie Tuck, The Uiversity of Adelaide. eotuck@iterode.o.et Dear Professor Erie Tuck. I i the previous letter (O AM 8:08:27) asked to direct resposes of reviewers which have served as the reaso for a deviatio of my paper: NEWTON'S SECOND LAW AND CURVILINEAR MOTION OF A MATERIAL PARTICLE to my address. However from Secretary Geeral ICTAM2008 I have received the iadequate aswer Thak you for your . Ufortuately the umber of papers submitted greatly exceeded the umber that could be accommodated i the program ad we regret to iform you that we caot accept your paper for presetatio. I ask you oce agai will direct resposes of reviewers to my address! Best regards, Yu. Zhivotov Last aswer to the Zhivotov's letter! ( :02:0) Dear Professor Zhivotov, Thak you agai for your . All papers for the cogress were reviewed by the Iteratioal Papers Committee appoited by IUTAM. As local orgaisers, we are ot ivolved i the review process or are we privy to their deliberatios. For these reasos I am uable to provide you with ay feedback from the Iteratioal Papers Committee. Best regards Jim Deier Cotiuatio o the followig page!

6 New aswer of Zhivotov! (Date: July 9, 2008) Presidet IUTAM Professor L.B. Freud Copy ICTAM 2008, Presidet Professor Erie Tuck Dear Presidet IUTAM, Professor L.B. Freud. I have addressed to orgaizers of cogress ICTAM 2008 with the request to give resposes of reviewers o a paper «NEWTON'S SECOND LAW AND CURVILINEAR TRANSLATIONAL MOTION OF THE BODY» (idetificatio umber 03). Prof. Jim Deier has iformed, that he has o resposes of reviewers ad orgaizers of the cogress have o feedback with Iteratioal Papers Committee. I hope, that the maagemet of the IUTAM has a feedback with Iteratioal Papers Committee. Therefore I ask you to assist i receptio of resposes of reviewers o my paper. Best regards Yu. Zhivotov P. S. I iform also, that the same history has happeed to a paper TORQUE EQUATION FOR RIGID ROTOR WITH ELASTIC SHAFT (ID 0856), which has bee set o the cogress ICTAM04. The give paper has bee published i magazie ad placed for the review Similar actios Iteratioal Papers Committee do ot promote promotio of mechaics.

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

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

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

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

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

Classical Mechanics Qualifying Exam Solutions Problem 1.

Classical Mechanics Qualifying Exam Solutions Problem 1. Jauary 4, Uiversity of Illiois at Chicago Departmet of Physics Classical Mechaics Qualifyig Exam Solutios Prolem. A cylider of a o-uiform radial desity with mass M, legth l ad radius R rolls without slippig

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

Systems of Particles: Angular Momentum and Work Energy Principle

Systems of Particles: Angular Momentum and Work Energy Principle 1 2.003J/1.053J Dyamics ad Cotrol I, Sprig 2007 Professor Thomas Peacock 2/20/2007 Lecture 4 Systems of Particles: Agular Mometum ad Work Eergy Priciple Systems of Particles Agular Mometum (cotiued) τ

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

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

Physics Supplement to my class. Kinetic Theory

Physics Supplement to my class. Kinetic Theory Physics Supplemet to my class Leaers should ote that I have used symbols for geometrical figures ad abbreviatios through out the documet. Kietic Theory 1 Most Probable, Mea ad RMS Speed of Gas Molecules

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

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

ES.182A Topic 40 Notes Jeremy Orloff

ES.182A Topic 40 Notes Jeremy Orloff ES.182A opic 4 Notes Jeremy Orloff 4 Flux: ormal form of Gree s theorem Gree s theorem i flux form is formally equivalet to our previous versio where the lie itegral was iterpreted as work. Here we will

More information

The Born-Oppenheimer approximation

The Born-Oppenheimer approximation The Bor-Oppeheimer approximatio 1 Re-writig the Schrödiger equatio We will begi from the full time-idepedet Schrödiger equatio for the eigestates of a molecular system: [ P 2 + ( Pm 2 + e2 1 1 2m 2m m

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

Fluid Physics 8.292J/12.330J % (1)

Fluid Physics 8.292J/12.330J % (1) Fluid Physics 89J/133J Problem Set 5 Solutios 1 Cosider the flow of a Euler fluid i the x directio give by for y > d U = U y 1 d for y d U + y 1 d for y < This flow does ot vary i x or i z Determie the

More information

NUMERICAL METHODS FOR SOLVING EQUATIONS

NUMERICAL METHODS FOR SOLVING EQUATIONS Mathematics Revisio Guides Numerical Methods for Solvig Equatios Page 1 of 11 M.K. HOME TUITION Mathematics Revisio Guides Level: GCSE Higher Tier NUMERICAL METHODS FOR SOLVING EQUATIONS Versio:. Date:

More information

TR/46 OCTOBER THE ZEROS OF PARTIAL SUMS OF A MACLAURIN EXPANSION A. TALBOT

TR/46 OCTOBER THE ZEROS OF PARTIAL SUMS OF A MACLAURIN EXPANSION A. TALBOT TR/46 OCTOBER 974 THE ZEROS OF PARTIAL SUMS OF A MACLAURIN EXPANSION by A. TALBOT .. Itroductio. A problem i approximatio theory o which I have recetly worked [] required for its solutio a proof that the

More information

MATH CALCULUS II Objectives and Notes for Test 4

MATH CALCULUS II Objectives and Notes for Test 4 MATH 44 - CALCULUS II Objectives ad Notes for Test 4 To do well o this test, ou should be able to work the followig tpes of problems. Fid a power series represetatio for a fuctio ad determie the radius

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

EXAM-3 MATH 261: Elementary Differential Equations MATH 261 FALL 2006 EXAMINATION COVER PAGE Professor Moseley

EXAM-3 MATH 261: Elementary Differential Equations MATH 261 FALL 2006 EXAMINATION COVER PAGE Professor Moseley EXAM-3 MATH 261: Elemetary Differetial Equatios MATH 261 FALL 2006 EXAMINATION COVER PAGE Professor Moseley PRINT NAME ( ) Last Name, First Name MI (What you wish to be called) ID # EXAM DATE Friday Ocober

More information

Chapter 1. Complex Numbers. Dr. Pulak Sahoo

Chapter 1. Complex Numbers. Dr. Pulak Sahoo Chapter 1 Complex Numbers BY Dr. Pulak Sahoo Assistat Professor Departmet of Mathematics Uiversity Of Kalyai West Begal, Idia E-mail : sahoopulak1@gmail.com 1 Module-2: Stereographic Projectio 1 Euler

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

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

3 Balance equations ME338A CONTINUUM MECHANICS

3 Balance equations ME338A CONTINUUM MECHANICS ME338A CONTINUUM MECHANICS lecture otes 1 thursy, may 1, 28 Basic ideas util ow: kiematics, i.e., geeral statemets that characterize deformatio of a material body B without studyig its physical cause ow:

More information

A NOTE ON THE TOTAL LEAST SQUARES FIT TO COPLANAR POINTS

A NOTE ON THE TOTAL LEAST SQUARES FIT TO COPLANAR POINTS A NOTE ON THE TOTAL LEAST SQUARES FIT TO COPLANAR POINTS STEVEN L. LEE Abstract. The Total Least Squares (TLS) fit to the poits (x,y ), =1,,, miimizes the sum of the squares of the perpedicular distaces

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

Name Solutions to Test 2 October 14, 2015

Name Solutions to Test 2 October 14, 2015 Name Solutios to Test October 4, 05 This test cosists of three parts. Please ote that i parts II ad III, you ca skip oe questio of those offered. The equatios below may be helpful with some problems. Costats

More information

1 of 7 7/16/2009 6:06 AM Virtual Laboratories > 6. Radom Samples > 1 2 3 4 5 6 7 6. Order Statistics Defiitios Suppose agai that we have a basic radom experimet, ad that X is a real-valued radom variable

More information

EF 151 Exam #4, Fall, 2010 Page 1 of 5

EF 151 Exam #4, Fall, 2010 Page 1 of 5 EF 5 Exam #4, Fall, 00 Page of 5 Name: Sectio: Guidelies: Assume 3 sigificat figures for all give umbers uless otherwise stated Show all of your work o work, o credit Write your fial aswer i the box provided

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

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

PHYS-505 Parity and other Discrete Symmetries Lecture-7!

PHYS-505 Parity and other Discrete Symmetries Lecture-7! PHYS-505 Parity ad other Discrete Symmetries Lecture-7! 1 Discrete Symmetries So far we have cosidered cotiuous symmetry operators that is, operatios that ca be obtaied by applyig successively ifiitesimal

More information

COURSE INTRODUCTION: WHAT HAPPENS TO A QUANTUM PARTICLE ON A PENDULUM π 2 SECONDS AFTER IT IS TOSSED IN?

COURSE INTRODUCTION: WHAT HAPPENS TO A QUANTUM PARTICLE ON A PENDULUM π 2 SECONDS AFTER IT IS TOSSED IN? COURSE INTRODUCTION: WHAT HAPPENS TO A QUANTUM PARTICLE ON A PENDULUM π SECONDS AFTER IT IS TOSSED IN? DROR BAR-NATAN Follows a lecture give by the author i the trivial otios semiar i Harvard o April 9,

More information

Definitions and Theorems. where x are the decision variables. c, b, and a are constant coefficients.

Definitions and Theorems. where x are the decision variables. c, b, and a are constant coefficients. Defiitios ad Theorems Remember the scalar form of the liear programmig problem, Miimize, Subject to, f(x) = c i x i a 1i x i = b 1 a mi x i = b m x i 0 i = 1,2,, where x are the decisio variables. c, b,

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

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

Differentiable Convex Functions

Differentiable Convex Functions Differetiable Covex Fuctios The followig picture motivates Theorem 11. f ( x) f ( x) f '( x)( x x) ˆx x 1 Theorem 11 : Let f : R R be differetiable. The, f is covex o the covex set C R if, ad oly if for

More information

The Space Redundant Robotic Manipulator Chaotic Motion Dynamics Control Algorithm

The Space Redundant Robotic Manipulator Chaotic Motion Dynamics Control Algorithm Sesors & rasducers, Vol. 75, Issue 7, July 24, pp. 27-3 Sesors & rasducers 24 by IFSA Publishig, S. L. http://www.sesorsportal.com he Space Redudat Robotic Maipulator Chaotic Motio Dyamics Cotrol Algorithm

More information

Fundamental Concepts: Surfaces and Curves

Fundamental Concepts: Surfaces and Curves UNDAMENTAL CONCEPTS: SURACES AND CURVES CHAPTER udametal Cocepts: Surfaces ad Curves. INTRODUCTION This chapter describes two geometrical objects, vi., surfaces ad curves because the pla a ver importat

More information

Lecture 8: Solving the Heat, Laplace and Wave equations using finite difference methods

Lecture 8: Solving the Heat, Laplace and Wave equations using finite difference methods Itroductory lecture otes o Partial Differetial Equatios - c Athoy Peirce. Not to be copied, used, or revised without explicit writte permissio from the copyright ower. 1 Lecture 8: Solvig the Heat, Laplace

More information

MATH 1A FINAL (7:00 PM VERSION) SOLUTION. (Last edited December 25, 2013 at 9:14pm.)

MATH 1A FINAL (7:00 PM VERSION) SOLUTION. (Last edited December 25, 2013 at 9:14pm.) MATH A FINAL (7: PM VERSION) SOLUTION (Last edited December 5, 3 at 9:4pm.) Problem. (i) Give the precise defiitio of the defiite itegral usig Riema sums. (ii) Write a epressio for the defiite itegral

More information

(c) Write, but do not evaluate, an integral expression for the volume of the solid generated when R is

(c) Write, but do not evaluate, an integral expression for the volume of the solid generated when R is Calculus BC Fial Review Name: Revised 7 EXAM Date: Tuesday, May 9 Remiders:. Put ew batteries i your calculator. Make sure your calculator is i RADIAN mode.. Get a good ight s sleep. Eat breakfast. Brig:

More information

REGRESSION (Physics 1210 Notes, Partial Modified Appendix A)

REGRESSION (Physics 1210 Notes, Partial Modified Appendix A) REGRESSION (Physics 0 Notes, Partial Modified Appedix A) HOW TO PERFORM A LINEAR REGRESSION Cosider the followig data poits ad their graph (Table I ad Figure ): X Y 0 3 5 3 7 4 9 5 Table : Example Data

More information

Formation of A Supergain Array and Its Application in Radar

Formation of A Supergain Array and Its Application in Radar Formatio of A Supergai Array ad ts Applicatio i Radar Tra Cao Quye, Do Trug Kie ad Bach Gia Duog. Research Ceter for Electroic ad Telecommuicatios, College of Techology (Coltech, Vietam atioal Uiversity,

More information

CALCULUS AB SECTION I, Part A Time 60 minutes Number of questions 30 A CALCULATOR MAY NOT BE USED ON THIS PART OF THE EXAM.

CALCULUS AB SECTION I, Part A Time 60 minutes Number of questions 30 A CALCULATOR MAY NOT BE USED ON THIS PART OF THE EXAM. AP Calculus AB Portfolio Project Multiple Choice Practice Name: CALCULUS AB SECTION I, Part A Time 60 miutes Number of questios 30 A CALCULATOR MAY NOT BE USED ON THIS PART OF THE EXAM. Directios: Solve

More information

Appendix: The Laplace Transform

Appendix: The Laplace Transform Appedix: The Laplace Trasform The Laplace trasform is a powerful method that ca be used to solve differetial equatio, ad other mathematical problems. Its stregth lies i the fact that it allows the trasformatio

More information

AP Calculus BC Review Applications of Derivatives (Chapter 4) and f,

AP Calculus BC Review Applications of Derivatives (Chapter 4) and f, AP alculus B Review Applicatios of Derivatives (hapter ) Thigs to Kow ad Be Able to Do Defiitios of the followig i terms of derivatives, ad how to fid them: critical poit, global miima/maima, local (relative)

More information

Notes The Incremental Motion Model:

Notes The Incremental Motion Model: The Icremetal Motio Model: The Jacobia Matrix I the forward kiematics model, we saw that it was possible to relate joit agles θ, to the cofiguratio of the robot ed effector T I this sectio, we will see

More information

Matsubara-Green s Functions

Matsubara-Green s Functions Matsubara-Gree s Fuctios Time Orderig : Cosider the followig operator If H = H the we ca trivially factorise this as, E(s = e s(h+ E(s = e sh e s I geeral this is ot true. However for practical applicatio

More information

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

Discrete Mathematics for CS Spring 2007 Luca Trevisan Lecture 22

Discrete Mathematics for CS Spring 2007 Luca Trevisan Lecture 22 CS 70 Discrete Mathematics for CS Sprig 2007 Luca Trevisa Lecture 22 Aother Importat Distributio The Geometric Distributio Questio: A biased coi with Heads probability p is tossed repeatedly util the first

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

Math 312 Lecture Notes One Dimensional Maps

Math 312 Lecture Notes One Dimensional Maps Math 312 Lecture Notes Oe Dimesioal Maps Warre Weckesser Departmet of Mathematics Colgate Uiversity 21-23 February 25 A Example We begi with the simplest model of populatio growth. Suppose, for example,

More information

Linear Regression Demystified

Linear Regression Demystified Liear Regressio Demystified Liear regressio is a importat subject i statistics. I elemetary statistics courses, formulae related to liear regressio are ofte stated without derivatio. This ote iteds to

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

Numerical Study on MHD Flow And Heat Transfer With The Effect Of Microrotational Parameter In The Porous Medium

Numerical Study on MHD Flow And Heat Transfer With The Effect Of Microrotational Parameter In The Porous Medium IOSR Joural of Egieerig (IOSRJEN) ISSN (e): 5-3, ISSN (p): 78-879 Vol. 5, Issue 4 (April. 5), V PP 8-7 www.iosrje.org Numerical Study o MHD Flow Ad Heat rasfer With he Effect Of Microrotatioal Parameter

More information

On Degeneracy of Lower Envelopes of Algebraic Surfaces

On Degeneracy of Lower Envelopes of Algebraic Surfaces CCCG 010, Wiipeg MB, August 9 11, 010 O Degeeracy of Lower Evelopes of Algebraic Surfaces Kimikazu Kato Abstract We aalyze degeeracy of lower evelopes of algebraic surfaces. We focus o the cases omitted

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

1. By using truth tables prove that, for all statements P and Q, the statement

1. By using truth tables prove that, for all statements P and Q, the statement Author: Satiago Salazar Problems I: Mathematical Statemets ad Proofs. By usig truth tables prove that, for all statemets P ad Q, the statemet P Q ad its cotrapositive ot Q (ot P) are equivalet. I example.2.3

More information

6 Integers Modulo n. integer k can be written as k = qn + r, with q,r, 0 r b. So any integer.

6 Integers Modulo n. integer k can be written as k = qn + r, with q,r, 0 r b. So any integer. 6 Itegers Modulo I Example 2.3(e), we have defied the cogruece of two itegers a,b with respect to a modulus. Let us recall that a b (mod ) meas a b. We have proved that cogruece is a equivalece relatio

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

Chapter 10: Power Series

Chapter 10: Power Series Chapter : Power Series 57 Chapter Overview: Power Series The reaso series are part of a Calculus course is that there are fuctios which caot be itegrated. All power series, though, ca be itegrated because

More information

Extended Electron in Constant Electric Field Part 1 : The net electric force Fe produced on the extended electron

Extended Electron in Constant Electric Field Part 1 : The net electric force Fe produced on the extended electron 1 Exteded Electro i Costat Electric Field Part 1 : The et electric force Fe produced o the exteded electro Hoa Va Nguye Email : hoaguye2312@yahoo.ca Abstract : Whe a exteded electro is subject to a exteral

More information

Upper bound for ropelength of pretzel knots

Upper bound for ropelength of pretzel knots Upper boud for ropelegth of pretzel kots Safiya Mora August 25, 2006 Abstract A model of the pretzel kot is described. A method for predictig the ropelegth of pretzel kots is give. A upper boud for the

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

A New Solution Method for the Finite-Horizon Discrete-Time EOQ Problem

A New Solution Method for the Finite-Horizon Discrete-Time EOQ Problem This is the Pre-Published Versio. A New Solutio Method for the Fiite-Horizo Discrete-Time EOQ Problem Chug-Lu Li Departmet of Logistics The Hog Kog Polytechic Uiversity Hug Hom, Kowloo, Hog Kog Phoe: +852-2766-7410

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

Mathematics Extension 1

Mathematics Extension 1 016 Bored of Studies Trial Eamiatios Mathematics Etesio 1 3 rd ctober 016 Geeral Istructios Total Marks 70 Readig time 5 miutes Workig time hours Write usig black or blue pe Black pe is preferred Board-approved

More information

Sequences and Series of Functions

Sequences and Series of Functions Chapter 6 Sequeces ad Series of Fuctios 6.1. Covergece of a Sequece of Fuctios Poitwise Covergece. Defiitio 6.1. Let, for each N, fuctio f : A R be defied. If, for each x A, the sequece (f (x)) coverges

More information

Chapter 5 Vibrational Motion

Chapter 5 Vibrational Motion Fall 4 Chapter 5 Vibratioal Motio... 65 Potetial Eergy Surfaces, Rotatios ad Vibratios... 65 Harmoic Oscillator... 67 Geeral Solutio for H.O.: Operator Techique... 68 Vibratioal Selectio Rules... 7 Polyatomic

More information

Balancing. Rotating Components Examples of rotating components in a mechanism or a machine. (a)

Balancing. Rotating Components Examples of rotating components in a mechanism or a machine. (a) alacig NOT COMPLETE Rotatig Compoets Examples of rotatig compoets i a mechaism or a machie. Figure 1: Examples of rotatig compoets: camshaft; crakshaft Sigle-Plae (Static) alace Cosider a rotatig shaft

More information

Axis Aligned Ellipsoid

Axis Aligned Ellipsoid Machie Learig for Data Sciece CS 4786) Lecture 6,7 & 8: Ellipsoidal Clusterig, Gaussia Mixture Models ad Geeral Mixture Models The text i black outlies high level ideas. The text i blue provides simple

More information

MEI Casio Tasks for Further Pure

MEI Casio Tasks for Further Pure Task Complex Numbers: Roots of Quadratic Equatios. Add a ew Equatio scree: paf 2. Chage the Complex output to a+bi: LpNNNNwd 3. Select Polyomial ad set the Degree to 2: wq 4. Set a=, b=5 ad c=6: l5l6l

More information

Warped, Chirp Z-Transform: Radar Signal Processing

Warped, Chirp Z-Transform: Radar Signal Processing arped, Chirp Z-Trasform: Radar Sigal Processig by Garimella Ramamurthy Report o: IIIT/TR// Cetre for Commuicatios Iteratioal Istitute of Iformatio Techology Hyderabad - 5 3, IDIA Jauary ARPED, CHIRP Z

More information

Polynomial Multiplication and Fast Fourier Transform

Polynomial Multiplication and Fast Fourier Transform Polyomial Multiplicatio ad Fast Fourier Trasform Com S 477/577 Notes Ya-Bi Jia Sep 19, 2017 I this lecture we will describe the famous algorithm of fast Fourier trasform FFT, which has revolutioized digital

More information

Z ß cos x + si x R du We start with the substitutio u = si(x), so du = cos(x). The itegral becomes but +u we should chage the limits to go with the ew

Z ß cos x + si x R du We start with the substitutio u = si(x), so du = cos(x). The itegral becomes but +u we should chage the limits to go with the ew Problem ( poits) Evaluate the itegrals Z p x 9 x We ca draw a right triagle labeled this way x p x 9 From this we ca read off x = sec, so = sec ta, ad p x 9 = R ta. Puttig those pieces ito the itegralrwe

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

CONTENTS. Course Goals. Course Materials Lecture Notes:

CONTENTS. Course Goals. Course Materials Lecture Notes: INTRODUCTION Ho Chi Mih City OF Uiversity ENVIRONMENTAL of Techology DESIGN Faculty Chapter of Civil 1: Orietatio. Egieerig Evaluatio Departmet of mathematical of Water Resources skill Egieerig & Maagemet

More information

Damped Vibration of a Non-prismatic Beam with a Rotational Spring

Damped Vibration of a Non-prismatic Beam with a Rotational Spring Vibratios i Physical Systems Vol.6 (0) Damped Vibratio of a No-prismatic Beam with a Rotatioal Sprig Wojciech SOCHACK stitute of Mechaics ad Fudametals of Machiery Desig Uiversity of Techology, Czestochowa,

More information

ACCESS TO SCIENCE, ENGINEERING AND AGRICULTURE: MATHEMATICS 1 MATH00030 SEMESTER / Statistics

ACCESS TO SCIENCE, ENGINEERING AND AGRICULTURE: MATHEMATICS 1 MATH00030 SEMESTER / Statistics ACCESS TO SCIENCE, ENGINEERING AND AGRICULTURE: MATHEMATICS 1 MATH00030 SEMESTER 1 018/019 DR. ANTHONY BROWN 8. Statistics 8.1. Measures of Cetre: Mea, Media ad Mode. If we have a series of umbers the

More information

BITSAT MATHEMATICS PAPER III. For the followig liear programmig problem : miimize z = + y subject to the costraits + y, + y 8, y, 0, the solutio is (0, ) ad (, ) (0, ) ad ( /, ) (0, ) ad (, ) (d) (0, )

More information

Analytical mechanics

Analytical mechanics Divisio of Mechaics Lud Uiversity Aalytical mechaics 7059 Name (write i block letters):. Id.-umber: Writte examiatio with five tasks. Please check that all tasks are icluded. A clea copy of the solutios

More information

(3) If you replace row i of A by its sum with a multiple of another row, then the determinant is unchanged! Expand across the i th row:

(3) If you replace row i of A by its sum with a multiple of another row, then the determinant is unchanged! Expand across the i th row: Math 5-4 Tue Feb 4 Cotiue with sectio 36 Determiats The effective way to compute determiats for larger-sized matrices without lots of zeroes is to ot use the defiitio, but rather to use the followig facts,

More information

Finally, we show how to determine the moments of an impulse response based on the example of the dispersion model.

Finally, we show how to determine the moments of an impulse response based on the example of the dispersion model. 5.3 Determiatio of Momets Fially, we show how to determie the momets of a impulse respose based o the example of the dispersio model. For the dispersio model we have that E θ (θ ) curve is give by eq (4).

More information

Machine Learning for Data Science (CS 4786)

Machine Learning for Data Science (CS 4786) Machie Learig for Data Sciece CS 4786) Lecture & 3: Pricipal Compoet Aalysis The text i black outlies high level ideas. The text i blue provides simple mathematical details to derive or get to the algorithm

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

Addition: Property Name Property Description Examples. a+b = b+a. a+(b+c) = (a+b)+c

Addition: Property Name Property Description Examples. a+b = b+a. a+(b+c) = (a+b)+c Notes for March 31 Fields: A field is a set of umbers with two (biary) operatios (usually called additio [+] ad multiplicatio [ ]) such that the followig properties hold: Additio: Name Descriptio Commutativity

More information

NATIONAL SENIOR CERTIFICATE GRADE 12

NATIONAL SENIOR CERTIFICATE GRADE 12 NATIONAL SENIOR CERTIFICATE GRADE MATHEMATICS P FEBRUARY/MARCH 009 MARKS: 50 TIME: 3 hours This questio paper cosists of 0 pages, a iformatio sheet ad 3 diagram sheets. Please tur over Mathematics/P DoE/Feb.

More information

A. Much too slow. C. Basically about right. E. Much too fast

A. Much too slow. C. Basically about right. E. Much too fast Geeral Questio 1 t this poit, we have bee i this class for about a moth. It seems like this is a good time to take stock of how the class is goig. g I promise ot to look at idividual resposes, so be cadid!

More information

w (1) ˆx w (1) x (1) /ρ and w (2) ˆx w (2) x (2) /ρ.

w (1) ˆx w (1) x (1) /ρ and w (2) ˆx w (2) x (2) /ρ. 2 5. Weighted umber of late jobs 5.1. Release dates ad due dates: maximimizig the weight of o-time jobs Oce we add release dates, miimizig the umber of late jobs becomes a sigificatly harder problem. For

More information

The type of limit that is used to find TANGENTS and VELOCITIES gives rise to the central idea in DIFFERENTIAL CALCULUS, the DERIVATIVE.

The type of limit that is used to find TANGENTS and VELOCITIES gives rise to the central idea in DIFFERENTIAL CALCULUS, the DERIVATIVE. NOTES : LIMITS AND DERIVATIVES Name: Date: Period: Iitial: LESSON.1 THE TANGENT AND VELOCITY PROBLEMS Pre-Calculus Mathematics Limit Process Calculus The type of it that is used to fid TANGENTS ad VELOCITIES

More information

Theorem: Let A n n. In this case that A does reduce to I, we search for A 1 as the solution matrix X to the matrix equation A X = I i.e.

Theorem: Let A n n. In this case that A does reduce to I, we search for A 1 as the solution matrix X to the matrix equation A X = I i.e. Theorem: Let A be a square matrix The A has a iverse matrix if ad oly if its reduced row echelo form is the idetity I this case the algorithm illustrated o the previous page will always yield the iverse

More information

IP Reference guide for integer programming formulations.

IP Reference guide for integer programming formulations. IP Referece guide for iteger programmig formulatios. by James B. Orli for 15.053 ad 15.058 This documet is iteded as a compact (or relatively compact) guide to the formulatio of iteger programs. For more

More information

Diploma Programme. Mathematics HL guide. First examinations 2014

Diploma Programme. Mathematics HL guide. First examinations 2014 Diploma Programme First eamiatios 014 33 Topic 6 Core: Calculus The aim of this topic is to itroduce studets to the basic cocepts ad techiques of differetial ad itegral calculus ad their applicatio. 6.1

More information

Uniform Strict Practical Stability Criteria for Impulsive Functional Differential Equations

Uniform Strict Practical Stability Criteria for Impulsive Functional Differential Equations Global Joural of Sciece Frotier Research Mathematics ad Decisio Scieces Volume 3 Issue Versio 0 Year 03 Type : Double Blid Peer Reviewed Iteratioal Research Joural Publisher: Global Jourals Ic (USA Olie

More information

Scheduling under Uncertainty using MILP Sensitivity Analysis

Scheduling under Uncertainty using MILP Sensitivity Analysis Schedulig uder Ucertaity usig MILP Sesitivity Aalysis M. Ierapetritou ad Zheya Jia Departmet of Chemical & Biochemical Egieerig Rutgers, the State Uiversity of New Jersey Piscataway, NJ Abstract The aim

More information

MATH 6101 Fall 2008 Newton and Differential Equations

MATH 6101 Fall 2008 Newton and Differential Equations MATH 611 Fall 8 Newto ad Differetial Equatios A Differetial Equatio What is a differetial equatio? A differetial equatio is a equatio relatig the quatities x, y ad y' ad possibly higher derivatives of

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