On General Solutions of First-Order Nonlinear Matrix and Scalar Ordinary Differential Equations

Similar documents
Boyce/DiPrima 9 th ed, Ch 2.1: Linear Equations; Method of Integrating Factors

Elementary Differential Equations and Boundary Value Problems

Let s look again at the first order linear differential equation we are attempting to solve, in its standard form:

On the Derivatives of Bessel and Modified Bessel Functions with Respect to the Order and the Argument

Midterm exam 2, April 7, 2009 (solutions)

General Article Application of differential equation in L-R and C-R circuit analysis by classical method. Abstract

DE Dr. M. Sakalli

FIRST-ORDER SYSTEMS OF ORDINARY DIFFERENTIAL EQUATIONS I: Introduction and Linear Systems

S.Y. B.Sc. (IT) : Sem. III. Applied Mathematics. Q.1 Attempt the following (any THREE) [15]

fiziks Institute for NET/JRF, GATE, IIT JAM, JEST, TIFR and GRE in PHYSICAL SCIENCES MATEMATICAL PHYSICS SOLUTIONS are

Lecture 1: Numerical Integration The Trapezoidal and Simpson s Rule

EXERCISE - 01 CHECK YOUR GRASP

On Ψ-Conditional Asymptotic Stability of First Order Non-Linear Matrix Lyapunov Systems

whereby we can express the phase by any one of the formulas cos ( 3 whereby we can express the phase by any one of the formulas

Spring 2006 Process Dynamics, Operations, and Control Lesson 2: Mathematics Review

Impulsive Differential Equations. by using the Euler Method

Transfer function and the Laplace transformation

An Indian Journal FULL PAPER. Trade Science Inc. A stage-structured model of a single-species with density-dependent and birth pulses ABSTRACT

2.1. Differential Equations and Solutions #3, 4, 17, 20, 24, 35

Charging of capacitor through inductor and resistor

( ) ( ) + = ( ) + ( )

Differential Equations

Lecture 4: Laplace Transforms

SOLUTIONS. 1. Consider two continuous random variables X and Y with joint p.d.f. f ( x, y ) = = = 15. Stepanov Dalpiaz

Lecture 1: Growth and decay of current in RL circuit. Growth of current in LR Circuit. D.K.Pandey

Logistic equation of Human population growth (generalization to the case of reactive environment).

H is equal to the surface current J S

CSE 245: Computer Aided Circuit Simulation and Verification

Math 3301 Homework Set 6 Solutions 10 Points. = +. The guess for the particular P ( ) ( ) ( ) ( ) ( ) ( ) ( ) cos 2 t : 4D= 2

Boyce/DiPrima 9 th ed, Ch 7.8: Repeated Eigenvalues

Feedback Control and Synchronization of Chaos for the Coupled Dynamos Dynamical System *

Intermediate Differential Equations Review and Basic Ideas

Wave Equation (2 Week)

Control System Engineering (EE301T) Assignment: 2

REPETITION before the exam PART 2, Transform Methods. Laplace transforms: τ dτ. L1. Derive the formulas : L2. Find the Laplace transform F(s) if.

Lecture 2: Current in RC circuit D.K.Pandey

UNIT #5 EXPONENTIAL AND LOGARITHMIC FUNCTIONS

5. An object moving along an x-coordinate axis with its scale measured in meters has a velocity of 6t

Institute of Actuaries of India

1 1 + x 2 dx. tan 1 (2) = ] ] x 3. Solution: Recall that the given integral is improper because. x 3. 1 x 3. dx = lim dx.

Final Exam : Solutions

MA 214 Calculus IV (Spring 2016) Section 2. Homework Assignment 1 Solutions

Undetermined coefficients for local fractional differential equations

5. Response of Linear Time-Invariant Systems to Random Inputs

Lecture 13 RC/RL Circuits, Time Dependent Op Amp Circuits

Section 3.5 Nonhomogeneous Equations; Method of Undetermined Coefficients

Asymptotic Solutions of Fifth Order Critically Damped Nonlinear Systems with Pair Wise Equal Eigenvalues and another is Distinct

1 Solutions to selected problems

Consider a system of 2 simultaneous first order linear equations

PERIODICAL SOLUTION OF SOME DIFFERENTIAL EQUATIONS UDC 517.9(045)=20. Julka Knežević-Miljanović

A Condition for Stability in an SIR Age Structured Disease Model with Decreasing Survival Rate

3.4 Repeated Roots; Reduction of Order

CPSC 211 Data Structures & Implementations (c) Texas A&M University [ 259] B-Trees

Chapter 3: Fourier Representation of Signals and LTI Systems. Chih-Wei Liu

ENGI 9420 Engineering Analysis Assignment 2 Solutions

System of Linear Differential Equations

Inverse Fourier Transform. Properties of Continuous time Fourier Transform. Review. Linearity. Reading Assignment Oppenheim Sec pp.289.

Phys463.nb Conductivity. Another equivalent definition of the Fermi velocity is

Theory of! Partial Differential Equations!

ANSWERS TO EVEN NUMBERED EXERCISES IN CHAPTER 11

A THREE COMPARTMENT MATHEMATICAL MODEL OF LIVER

NEW APPLICATIONS OF THE ABEL-LIOUVILLE FORMULA

Chapter 12 Introduction To The Laplace Transform

Mundell-Fleming I: Setup

Sections 2.2 & 2.3 Limit of a Function and Limit Laws

Inextensible flows of S s surfaces of biharmonic

Solutions of Sample Problems for Third In-Class Exam Math 246, Spring 2011, Professor David Levermore

Math 36. Rumbos Spring Solutions to Assignment #6. 1. Suppose the growth of a population is governed by the differential equation.

LaPlace Transform in Circuit Analysis

CHAPTER 9 Compressible Flow

AR(1) Process. The first-order autoregressive process, AR(1) is. where e t is WN(0, σ 2 )

Chapter 6 Differential Equations and Mathematical Modeling

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

1 st order ODE Initial Condition

Chapter 5 The Laplace Transform. x(t) input y(t) output Dynamic System

dt = C exp (3 ln t 4 ). t 4 W = C exp ( ln(4 t) 3) = C(4 t) 3.

Y 0.4Y 0.45Y Y to a proper ARMA specification.

Math Final Exam Solutions

t + t sin t t cos t sin t. t cos t sin t dt t 2 = exp 2 log t log(t cos t sin t) = Multiplying by this factor and then integrating, we conclude that

Math 333 Problem Set #2 Solution 14 February 2003

Poisson process Markov process

DEPARTMENT OF ELECTRICAL &ELECTRONICS ENGINEERING SIGNALS AND SYSTEMS. Assoc. Prof. Dr. Burak Kelleci. Spring 2018

Chapter 2. First Order Scalar Equations

Recall that by Theorems 10.3 and 10.4 together provide us the estimate o(n2 ), S(q) q 9, q=1

8. Basic RL and RC Circuits

Nonlocal Symmetries and Exact Solutions for PIB Equation

Chapter 8 The Complete Response of RL and RC Circuits

Math 334 Test 1 KEY Spring 2010 Section: 001. Instructor: Scott Glasgow Dates: May 10 and 11.

Math 23 Spring Differential Equations. Final Exam Due Date: Tuesday, June 6, 5pm

Voltage v(z) ~ E(z)D. We can actually get to this wave behavior by using circuit theory, w/o going into details of the EM fields!

Ministry of Education and Science of Ukraine National Technical University Ukraine "Igor Sikorsky Kiev Polytechnic Institute"

Theory of! Partial Differential Equations-I!

C From Faraday's Law, the induced voltage is, C The effect of electromagnetic induction in the coil itself is called selfinduction.

XV Exponential and Logarithmic Functions

EXISTENCE OF NON-OSCILLATORY SOLUTIONS TO FIRST-ORDER NEUTRAL DIFFERENTIAL EQUATIONS

SUPERCRITICAL BRANCHING DIFFUSIONS IN RANDOM ENVIRONMENT

t 2 B F x,t n dsdt t u x,t dxdt

Chapter 3 Boundary Value Problem

Math 2214 Solution Test 1B Fall 2017

Point Processes, Week 3, Wednesday

Transcription:

saartvlos mcnirbata rovnuli akadmiis moamb 3 #2 29 BULLTN OF TH ORN NTONL DMY OF SNS vol 3 no 2 29 Mahmaics On nral Soluions of Firs-Ordr Nonlinar Mari and Scalar Ordinary Diffrnial uaions uram L Kharaishvili cadmy Mmbr orian Naional cadmy of Scincs BSTRT This aricl conains h formula of nral soluions for paricular classs of firs-ordr nonlinar mari and scalar ordinary diffrnial uaions 29 Bull or Nal cad Sci Ky words: nral soluions firs ordr mari scalar nonlinar mari and scalar ordinary diffrnial uaions Firs-Ordr anonical Nonlinar uaion Problm Samn L us considr an uaion d p h F ] 2[ ] [ p d whr = F=F ar ivn n n marics wih coninuous lmns on h inrval h=h is a ivn arbirary admissibl n n mari funcion is an unknown n n mari Hr and vrywhr an admissibl funcion will b calld any funcion in rspc o which opraions prsnd in h aricl ar valid on h whol inrval Dfiniion Th soluion of uaion will b calld mari funcion = dfind on h inrval subsiuion of which in uaion is admissibl as a rsul of which w h idniy Dfiniion 2 L b an arbirary fid poin of h inrval and b arbirary fid consan of mari n n Mari funcion dfind on h inrval and dpndin on arbirary consan of mari n n will b calld h nral soluion of uaion if is a soluion of uaion saisfyin h iniial condiion = Th basic problm consiss in consrucin h nral soluion of uaion 2 Rular Marics Main Thorms To consruc h nral soluion of uaion w shall nd a mari funcion of rular mari Dfiniion 3 Mari R=R wih coninuous lmns i j n will b calld a rular mari if hr iss n n mari funcion Rd dfini coninuous and coninuously diffrniabl wih rspc o on r i j h inrval saisfyin h condiions: whr is a uni mari p Rd= R Rd; Rd Rd Rd Rd Rd 29 Bull or Nal cad Sci

6 uram L Kharaishvili Thorm Basic Thorm f h mari = is rular and h admissibl mari funcion = saisfis h condiion h d dfd hn is a soluion of uaion Proof W hav ph d dfd F i Ph h F Thorm is provd L h= whr = = ar arbirary admissibl funcions From Thorm i follows Thorm 2 L h mari = is rular = = ar arbirary admissibl scalar funcions and i f hr iss h admissibl mari funcion d dfd 2 hn mari funcion 2 is h nral soluion of h uaion p F 3 Proof From formula 2 i follows d dfd onsunly s Thorm mari funcion 2 is a soluion of uaion 3 L b an arbirary fid poin of h inrval and b an arbirary fid consan of mari n n ssum ha = Thn from formula 2 i follows d d Fd Thorm 2 is provd From Thorm i follows Thorm 3 L h mari = is rular = = ar arbirary admissibl funcions and i f hr iss h admissibl mari funcion d dfd hn mari funcion 4 is h nral soluion of h uaion p [ ] F 5 Proof From formula 4 i follows d dfd onsunly s Thorm mari funcion 4 is a soluion of h uaion 5 L b an arbirary fid poin of h inrval and b an arbirary fid consan of mari n n ssum ha = Thn from formula 4 i follows Thorm 3 is provd d dfd 4

On nral Soluions of Firs-Ordr Nonlinar Mari and Scalar Ordinary Diffrnial uaions 7 3 riria of Rulariy Thorm 4 ririon of Rulariy L i j b an arbirary n n mari wih coninuous and coninuously diffrniabl lmns i j i j n on h inrval L k k P a a a whr m k ar arbirary coninuous and coninuously diffrniabl scalar funcions L d P L R P P rular Hr h do sands for h drivaiv d/d Proof W hav a m and Rd P Rd P and Rd P RP R Rd Thn mari R is Thorm 4 is provd orollary ririon of Rulariy L k a a d R and Rd Thn mari R is rular 4 pplicaions 4 nral Soluions of Firs Ordr Nonlinar Scalar Diffrnial uaions L us considr h uaion p-a =f 6 whr a=a f=f = = ar ivn arbirary admissibl scalar funcions f n= from Thorm 2 i follows Rsul f a=a f=f = = ar arbirary admissibl scalar funcions and i hn h nral soluion of h uaion a f 7 Rmark n his cas For ampl h nral soluion of h uaion whr a=a f=f = f c fd a ar arbirary admissibl funcions c fd Rmark n his cas = - f h nral soluion of h uaion f a a d a d c f d 8

8 uram L Kharaishvili f n = from Thorm 3 i follows Rsul 2 f a=a f=f = = ar arbirary admissibl scalar funcions and i hn h nral soluion of h uaion a f a 9 fd c For ampl h nral soluion of h uaion sc a f a whr a=a f=f = ar arbirary admissibl funcions arcsin fd c Rmark 2 n his cas =sin 5 Nonlinar Mari Diffrnial uaions ampls ampl L whr ar arbirary admissibl funcions L and i From orollary i follows ha mari is rular if d L us considr h mari funcion d W hav s [] d Hnc d d d and mari is rular L us considr h uaion 3 whr ar arbirary admissibl funcions From Thorm 2 i follows 2 Fd c For ampl if cons F w hav

On nral Soluions of Firs-Ordr Nonlinar Mari and Scalar Ordinary Diffrnial uaions 9 [] is From h uaion 3 i follows P onsunly h paricular soluion of h uaion p whr ar arbirary admissibl funcions cons ampl 2 L whr ar arbirary admissibl funcions L i Hnc mari is rular if d L us considr h mari funcion d W hav s [] d i d and mari is rular L us considr uaion 5 whr is an arbirary admissibl scalar funcion f hn from Thorm 3 i follows ha h nral soluion of uaion 5 Fd d d i 2 Fd For ampl l F W hav

uram L Kharaishvili matmaika pirvli riis arawrfivi skalaruli da mariculi vulbrivi difrncialuri anolbbis zoadi amonasnbis Ssab araisvili akadmikosi saartvlos mcnirbata rovnuli akadmia saiasi dadnilia zoadi amonasnbis formulbi pirvli riis arawrfivi skalaruli da mariculi vulbrivi difrncialuri anolbbis krzo klasbisatvis RFRNS uram L Kharaishvili 27 Bull or Nal cad Sci 75 : 7-22 2 Nicolai Kudryashov 998 JPhys: Mah n 3 6 3 M Ndljkov D Rajr 2 Novisad J Mah 3 4 D Majiros 978 Ukrainskii Mam Zhurnal 3 2 Rcivd pril 29 onsunly s [] if ] [ ] [ Hnc h paricular soluion of h uaion p whr ar arbirary admissibl funcions n conclusion w mus noic ha h rlad problms ar invsiad in [2-4]