ON SOME PROPERTIES OF THE SYMPLECTIC AND HAMILTONIAN MATRICES

Size: px
Start display at page:

Download "ON SOME PROPERTIES OF THE SYMPLECTIC AND HAMILTONIAN MATRICES"

Transcription

1 Proceedings of he Inernaional Conference on Theory and Applicaions of Mahemaics and Informaics - ICTAMI 2004, Thessaloniki, Greece ON SOME PROPERTIES OF THE SYMPLECTIC AND HAMILTONIAN MATRICES by Dorin Wainberg Absrac: In he firs par of he paper he symplecic and Hamilonian marices are defined and some properies are poined, and in he second par a relaion beween hose wo ses of marices is proved. 1. Proprieies of symplecic and Hamilonian marices For he beginning i will be inroduced he square mari J M 2 n 2n ( ) defined by 0n I n J = (1) I n 0n where: 0n M n n ( ) zero mari I M n ( ) ideniy mari n n Remark 1 I is no very complicaed o prove ha he ne properies of he mari J are real (properies ha will be very useful o prove some proposiions ha follow): i) J = -J J ii) J -1 = iii) J J = I 2 n iv) J J = - I 2 n 2 v) J = - I 2 n vi) de J = ± 1 Now he definiion of he symplecic and Hamilonian marices are given: Definiion 1 A mari A M 2 n 2n ( ) is called symplecic if: A J A = J (2) 442

2 Dorin Wainberg - On some properies of he symplecic and Hamilonian marices where J M 2 n 2n ( ) is from (1). We will denoe by SP(n, ) no = { A M 2 n 2n ( ) A J A = J } he se of 2n 2n real symplecic marices. Definiion 2 A mari A M 2 n 2n ( ) is called Hamilonian if: A J + JA = 0 (3) where J M 2 n 2n ( ) is from (1). We will denoe by sp(n, ) no = { A M 2 n 2n ( ) A J + JA = 0 } he se of 2n 2n real Hamilonian marices. In he ne par some properies of hose ses of marices will be proved, for eample: Proposiion 1 Le A, B SP(n, ). The ne relaions are rue: a) A is nonsingular; b) A -1 = - J A J; c) A, A -1, AB SP(n, ). a) From he definiion of symplecic marices we have A J A = J de( A JA) = de J de de J de A = de J de A de A = 1 2 (de A ) = 1 de A = ± 1 0 A is nonsingular. A b) A SP(n, ) A J A = J J A J = A -1 A A J = J A -1 J -1 A J = A -1 J =J J =J A -1 = - J A J. More, we have: A = - J A -1 J. c) A SP(n, ) A J A = J J A J A J = 2 J = - I 2 n A A J A J A = - A Now, muliplying a he lef side by (A ) -1, we will obain: J A J A = - I 2 n. Muliplying again a he righ side by J : A J A = - J = -(-J) = J A J A = J (A ) J A = J A SP(n, ) We will proof now ha A -1 SP(n, ). Using he relaion A -1 = - J A J (from he poin b)) we have successive: (A -1 ) J A -1 = (- J A J) J (- J A J) = 443

3 Dorin Wainberg - On some properies of he symplecic and Hamilonian marices = J (J A) J J A J = J 2 = - I 2 n = J A J (- I 2 n ) A J = = - J A J A J = A J A = (A J A) = = - J J J = J J = - I 2 n = J A -1 SP(n, ) We will proof now ha AB SP(n, ): (AB) J AB = B A J A B = A J A = J = B J B = = J AB SP(n, ) Consequence. The se of symplecic marices SP(n, ) is a subgroup of he se of nonsingular marices GL(n, ) repored o muliplicaion. Indeed we have AB SP(n, ), A, B SP(n, ), and AB -1 SP(n, ), A, B SP(n, ). Proposiion 2 Le A SP(n, ) and p A () - he characerisic polynomial of he mari A. If p A (c) = 0, hen p A ( 1 ) = p (c) c A = p A ( 1 ) = 0, where c. c p A () = de(a I 2 n ) = A = - J A -1 J = de(- J A -1 J I 2 n ) = I 2 n = - J 2 = de( J( - A -1 ) J + J 2 ) = = de( J( - A -1 + I 2 n ) J ) = = de J de( - A -1 + I 2 n ) de J = de J = ± 1 = de( - A -1 + I 2 n ) = = de( - A -1 + AA -1 ) = = de( - I 2 n + A ) de( A -1 )= = ± de(a - I 2 n ) = ± 2n de(a - 1 I 2 n ) = ± 2n p A ( 1 ) 2n p A ( 1 ) = 0 p ) A ( 1 = 0 p ) A ( 1 = 0 p (c) c A = 0 p A ( 1 ) = 0. c Proposiion 3 The ne relaions are equivalen: a) A is a Hamilonian mari; b) A = JS, where S = S ; c) ( JA ) = JA. 444 J

4 Dorin Wainberg - On some properies of he symplecic and Hamilonian marices a b A = J J J = I2n J A A = J(- J)A A sp( n, R) ( J(- JA)) J + JA = 0 (- JA) = - JA (- JA) = - JA J(- JA) = A If - JA = S A = J(- JA) = J(- JA) A = JS = J S S = a c A J + JA = 0 A J = - JA JA = - ( JA ) ( JA ) = JA S. J J ( ) (A J) = (- JA) J A = - ( JA ) - Proposiion 4 Le A, B sp(n, ). The ne relaions are rue: a) A + B sp(n, ); b) α A sp(n, ), α ; c) [A, B] sp(n, ), where [A, B] def = AB BA a) Because A and B are Hamilonian marices i resuls ha A J + JA = 0 respecively B J + JB = 0. By adding hose wo relaions we will obain: (A + B ) J + J(A + B) = 0 (A + B) J + J(A + B) = 0 A + B sp(n, ). ii) A J + JA = 0 α A J α + JA α = 0 A α J + J(A α ) = 0 (A α ) J + J(A α ) = 0 α A sp(n, ). iii) We will prove ha [A, B] = J M, where M = M. We know ha A = JS and B = JR, where S = S and R = R. [A, B] = AB BA = JSJR JRJS = J(SJR RJS), from where, making he noaion SJR RJS = M we will obain [A, B] = J M. M Now we will show ha M = M = (SJR RJS) = (SJR) (RJS) = R J S S J R = - RJS + SJR = SJR RJS = M Consequence. ( sp(n, ), [, ] ) is a Lie algebra.. We will prove he necessary properies of he bracke [, ] : bilineariy, anisymmery and Jacobi s relaion. 445

5 Dorin Wainberg - On some properies of he symplecic and Hamilonian marices i) [ αa + βb, C] = α[a, C] + β[b, C] - evidenly he operaion is bilinear. ii) [A, B] = AB BA = - (BA AB) = - [B, A] he operaion is anisymmeric. iii) Jacobi s relaion is saisfied: [[A, B], C] + [[C, A], B] + [[B, C], A] = [AB BA, C] + [CA AC, B] + [BC CB, A] = =ABC BAC (CAB CBA) + CAB ACB (BCA BAC) + BCA CBA (ABC ACB) = 0 Proposiion 5 Le A sp(n, ) and p A () - he characerisic polynomial of he mari A. Then: a) p A () = p A ( ) b) if p A (c) = 0, hen p A ( c) = p A (c) = p A ( c) = 0, where c. a) p A () = de(a I 2n ), bu A = J A J p A () = de(j A J I 2n ) A = - J A -1 J = de(j A J J J) = = de( J( A + I 2n )J ) = = de J de(a + I 2n )de J = de J = ± 1 = de(a + I 2n ) = de(a + I 2n ) = = de(a + I 2n ) = = de(a + I 2n ) = de(a ( ) I 2n ) = p A ( ) b) p A (c) = 0 a) p A ( c) = 0. p A () is a real coefficiens polynomial p A (c) = 0 p A ( c) = 0. 2.A relaion beween he ses sp(n, ) and SP(n, ) Theorem: Le A M 2 n 2n ( ). The ne relaions are equivalen: a. A sp (n, ) b. ep (A) SP (n, ) a b A sp (n, ) A J + JA = O 446 a)

6 Dorin Wainberg - On some properies of he symplecic and Hamilonian marices Le U() = (ep(a)) J ep(a) Bu, on he oher hand we have: du d = [ ep(a)] J ep(a) + [ep(a)] d J [ ep(a)] d d d = [A ep(a)] J ep(a) + [ep(a)] J A (ep(a)) = [ep(a)] A J ep (A) + [ep(a)] JA ep(a) = [ep(a)] [A J + J A] ep (A) = 0. U() consan. ( * ) Bu U(0) = (ep(a Α O)) J ep(a Α O) = J ( ** ) From ( * ) and ( ** ) U () = 0 (ep(a)) J ep(a) = J ep(a) SP (n, ). b a ep (A) sp (n, ) (ep (A)) Α J Α ep (A) = J. d [(ep(a)) J Α (ep (A))] = 0 d d [ ep (A)] J ep (A) + (ep (A)) d J [ ep (A)] = 0 d d (A ep(a)) J ep(a) + (ep(a)) J A ep(a) = 0 (ep(a)) A J ep(a) + (ep(a)) J A ep(a) = 0 (ep(a)) [A J + JA] ep(a) = 0 Muliplying a he righ by ((ep (A)) ) -1 and a he lef by (ep (A)) -1 we will obain: A J + JA = 0 A sp (n, ). References: [1] Mircea Pua Calcul mariceal, Timişoara, Ediura Miron, 2000 [2] Mircea Pua Varieăţi diferenţiabile - probleme, Timişoara, Ediura Miron, 2002 [3] Mircea Pua Hamilonian Mechanical Sysems and Geomeric Quaninizaion, Kluwer, [4] R. Abraham, J. Marsden and T. Raiu - Manifolds, Tensor Analysis and Applicaions, Second Ediion, Applied Mah. Sciences 75, Springer Verlag, Auhor: 447

7 Dorin Wainberg - On some properies of he symplecic and Hamilonian marices Dorin Wainberg, 1 Decembrie 1918 Universiy of Alba Iulia, address: wainbergdorin@yahoo.com 448

Hamiltonian Matrices and the Algebraic Riccati Equation. Seminar presentation

Hamiltonian Matrices and the Algebraic Riccati Equation. Seminar presentation Hamiltonian Matrices and the Algebraic Riccati Equation Seminar presentation by Piyapong Yuantong 7th December 2009 Technische Universität Chemnitz 1 Hamiltonian matrices We start by introducing the square

More information

THE GENERALIZED PASCAL MATRIX VIA THE GENERALIZED FIBONACCI MATRIX AND THE GENERALIZED PELL MATRIX

THE GENERALIZED PASCAL MATRIX VIA THE GENERALIZED FIBONACCI MATRIX AND THE GENERALIZED PELL MATRIX J Korean Mah Soc 45 008, No, pp 479 49 THE GENERALIZED PASCAL MATRIX VIA THE GENERALIZED FIBONACCI MATRIX AND THE GENERALIZED PELL MATRIX Gwang-yeon Lee and Seong-Hoon Cho Reprined from he Journal of he

More information

Math 315: Linear Algebra Solutions to Assignment 6

Math 315: Linear Algebra Solutions to Assignment 6 Mah 35: Linear Algebra s o Assignmen 6 # Which of he following ses of vecors are bases for R 2? {2,, 3, }, {4,, 7, 8}, {,,, 3}, {3, 9, 4, 2}. Explain your answer. To generae he whole R 2, wo linearly independen

More information

Matrix Versions of Some Refinements of the Arithmetic-Geometric Mean Inequality

Matrix Versions of Some Refinements of the Arithmetic-Geometric Mean Inequality Marix Versions of Some Refinemens of he Arihmeic-Geomeric Mean Inequaliy Bao Qi Feng and Andrew Tonge Absrac. We esablish marix versions of refinemens due o Alzer ], Carwrigh and Field 4], and Mercer 5]

More information

THE BERNOULLI NUMBERS. t k. = lim. = lim = 1, d t B 1 = lim. 1+e t te t = lim t 0 (e t 1) 2. = lim = 1 2.

THE BERNOULLI NUMBERS. t k. = lim. = lim = 1, d t B 1 = lim. 1+e t te t = lim t 0 (e t 1) 2. = lim = 1 2. THE BERNOULLI NUMBERS The Bernoulli numbers are defined here by he exponenial generaing funcion ( e The firs one is easy o compue: (2 and (3 B 0 lim 0 e lim, 0 e ( d B lim 0 d e +e e lim 0 (e 2 lim 0 2(e

More information

Fractional Method of Characteristics for Fractional Partial Differential Equations

Fractional Method of Characteristics for Fractional Partial Differential Equations Fracional Mehod of Characerisics for Fracional Parial Differenial Equaions Guo-cheng Wu* Modern Teile Insiue, Donghua Universiy, 188 Yan-an ilu Road, Shanghai 51, PR China Absrac The mehod of characerisics

More information

t is a basis for the solution space to this system, then the matrix having these solutions as columns, t x 1 t, x 2 t,... x n t x 2 t...

t is a basis for the solution space to this system, then the matrix having these solutions as columns, t x 1 t, x 2 t,... x n t x 2 t... Mah 228- Fri Mar 24 5.6 Marix exponenials and linear sysems: The analogy beween firs order sysems of linear differenial equaions (Chaper 5) and scalar linear differenial equaions (Chaper ) is much sronger

More information

POSITIVE SOLUTIONS OF NEUTRAL DELAY DIFFERENTIAL EQUATION

POSITIVE SOLUTIONS OF NEUTRAL DELAY DIFFERENTIAL EQUATION Novi Sad J. Mah. Vol. 32, No. 2, 2002, 95-108 95 POSITIVE SOLUTIONS OF NEUTRAL DELAY DIFFERENTIAL EQUATION Hajnalka Péics 1, János Karsai 2 Absrac. We consider he scalar nonauonomous neural delay differenial

More information

2 Some Property of Exponential Map of Matrix

2 Some Property of Exponential Map of Matrix Soluion Se for Exercise Session No8 Course: Mahemaical Aspecs of Symmeries in Physics, ICFP Maser Program for M 22nd, January 205, a Room 235A Lecure by Amir-Kian Kashani-Poor email: kashani@lpensfr Exercise

More information

Oscillation of an Euler Cauchy Dynamic Equation S. Huff, G. Olumolode, N. Pennington, and A. Peterson

Oscillation of an Euler Cauchy Dynamic Equation S. Huff, G. Olumolode, N. Pennington, and A. Peterson PROCEEDINGS OF THE FOURTH INTERNATIONAL CONFERENCE ON DYNAMICAL SYSTEMS AND DIFFERENTIAL EQUATIONS May 4 7, 00, Wilmingon, NC, USA pp 0 Oscillaion of an Euler Cauchy Dynamic Equaion S Huff, G Olumolode,

More information

Roughness in ordered Semigroups. Muhammad Shabir and Shumaila Irshad

Roughness in ordered Semigroups. Muhammad Shabir and Shumaila Irshad World Applied Sciences Journal 22 (Special Issue of Applied Mah): 84-105, 2013 ISSN 1818-4952 IDOSI Publicaions, 2013 DOI: 105829/idosiwasj22am102013 Roughness in ordered Semigroups Muhammad Shabir and

More information

A New Kind of Fuzzy Sublattice (Ideal, Filter) of A Lattice

A New Kind of Fuzzy Sublattice (Ideal, Filter) of A Lattice nernaional Journal of Fuzzy Sysems Vol 3 No March 2 55 A New Kind of Fuzzy Sublaice (deal Filer) of A Laice B Davvaz O Kazanci Absrac Our aim in his paper is o inroduce sudy a new sor of fuzzy sublaice

More information

On fuzzy normed algebras

On fuzzy normed algebras Available online a www.jnsa.com J. Nonlinear Sci. Appl. 9 (2016), 5488 5496 Research Aricle On fuzzy normed algebras Tudor Bînzar a,, Flavius Paer a, Sorin Nădăban b a Deparmen of Mahemaics, Poliehnica

More information

GCD AND LCM-LIKE IDENTITIES FOR IDEALS IN COMMUTATIVE RINGS

GCD AND LCM-LIKE IDENTITIES FOR IDEALS IN COMMUTATIVE RINGS GCD AND LCM-LIKE IDENTITIES FOR IDEALS IN COMMUTATIVE RINGS D. D. ANDERSON, SHUZO IZUMI, YASUO OHNO, AND MANABU OZAKI Absrac. Le A 1,..., A n n 2 be ideals of a commuaive ring R. Le Gk resp., Lk denoe

More information

Chapter 2. First Order Scalar Equations

Chapter 2. First Order Scalar Equations Chaper. Firs Order Scalar Equaions We sar our sudy of differenial equaions in he same way he pioneers in his field did. We show paricular echniques o solve paricular ypes of firs order differenial equaions.

More information

Then. 1 The eigenvalues of A are inside R = n i=1 R i. 2 Union of any k circles not intersecting the other (n k)

Then. 1 The eigenvalues of A are inside R = n i=1 R i. 2 Union of any k circles not intersecting the other (n k) Ger sgorin Circle Chaper 9 Approimaing Eigenvalues Per-Olof Persson persson@berkeley.edu Deparmen of Mahemaics Universiy of California, Berkeley Mah 128B Numerical Analysis (Ger sgorin Circle) Le A be

More information

THE GEOMETRY MONOID OF AN IDENTITY

THE GEOMETRY MONOID OF AN IDENTITY THE GEOMETRY MONOID OF AN IDENTITY Parick DEHORNOY Universié decaen Main idea: For each algebraic ideniy I, (more generally, for each family of algebraic ideniy, acually for each equaional variey), here

More information

Two Properties of Catalan-Larcombe-French Numbers

Two Properties of Catalan-Larcombe-French Numbers 3 7 6 3 Journal of Ineger Sequences, Vol. 9 06, Aricle 6.3. Two Properies of Caalan-Larcombe-French Numbers Xiao-Juan Ji School of Mahemaical Sciences Soochow Universiy Suzhou Jiangsu 5006 P. R. China

More information

The Miki-type identity for the Apostol-Bernoulli numbers

The Miki-type identity for the Apostol-Bernoulli numbers Annales Mahemaicae e Informaicae 46 6 pp. 97 4 hp://ami.ef.hu The Mii-ype ideniy for he Aposol-Bernoulli numbers Orli Herscovici, Toufi Mansour Deparmen of Mahemaics, Universiy of Haifa, 3498838 Haifa,

More information

Robust estimation based on the first- and third-moment restrictions of the power transformation model

Robust estimation based on the first- and third-moment restrictions of the power transformation model h Inernaional Congress on Modelling and Simulaion, Adelaide, Ausralia, 6 December 3 www.mssanz.org.au/modsim3 Robus esimaion based on he firs- and hird-momen resricions of he power ransformaion Nawaa,

More information

Solution of Integro-Differential Equations by Using ELzaki Transform

Solution of Integro-Differential Equations by Using ELzaki Transform Global Journal of Mahemaical Sciences: Theory and Pracical. Volume, Number (), pp. - Inernaional Research Publicaion House hp://www.irphouse.com Soluion of Inegro-Differenial Equaions by Using ELzaki Transform

More information

Undetermined coefficients for local fractional differential equations

Undetermined coefficients for local fractional differential equations Available online a www.isr-publicaions.com/jmcs J. Mah. Compuer Sci. 16 (2016), 140 146 Research Aricle Undeermined coefficiens for local fracional differenial equaions Roshdi Khalil a,, Mohammed Al Horani

More information

arxiv:math/ v1 [math.nt] 3 Nov 2005

arxiv:math/ v1 [math.nt] 3 Nov 2005 arxiv:mah/0511092v1 [mah.nt] 3 Nov 2005 A NOTE ON S AND THE ZEROS OF THE RIEMANN ZETA-FUNCTION D. A. GOLDSTON AND S. M. GONEK Absrac. Le πs denoe he argumen of he Riemann zea-funcion a he poin 1 + i. Assuming

More information

Inequality measures for intersecting Lorenz curves: an alternative weak ordering

Inequality measures for intersecting Lorenz curves: an alternative weak ordering h Inernaional Scienific Conference Financial managemen of Firms and Financial Insiuions Osrava VŠB-TU of Osrava, Faculy of Economics, Deparmen of Finance 7 h 8 h Sepember 25 Absrac Inequaliy measures for

More information

Math-Net.Ru All Russian mathematical portal

Math-Net.Ru All Russian mathematical portal Mah-Ne.Ru All Russian mahemaical poral Aleksei S. Rodin, On he srucure of singular se of a piecewise smooh minimax soluion of Hamilon-Jacobi-Bellman equaion, Ural Mah. J., 2016, Volume 2, Issue 1, 58 68

More information

An Invariance for (2+1)-Extension of Burgers Equation and Formulae to Obtain Solutions of KP Equation

An Invariance for (2+1)-Extension of Burgers Equation and Formulae to Obtain Solutions of KP Equation Commun Theor Phys Beijing, China 43 2005 pp 591 596 c Inernaional Academic Publishers Vol 43, No 4, April 15, 2005 An Invariance for 2+1-Eension of Burgers Equaion Formulae o Obain Soluions of KP Equaion

More information

An Introduction to Malliavin calculus and its applications

An Introduction to Malliavin calculus and its applications An Inroducion o Malliavin calculus and is applicaions Lecure 5: Smoohness of he densiy and Hörmander s heorem David Nualar Deparmen of Mahemaics Kansas Universiy Universiy of Wyoming Summer School 214

More information

Two Coupled Oscillators / Normal Modes

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

More information

14 Autoregressive Moving Average Models

14 Autoregressive Moving Average Models 14 Auoregressive Moving Average Models In his chaper an imporan parameric family of saionary ime series is inroduced, he family of he auoregressive moving average, or ARMA, processes. For a large class

More information

Distance Between Two Ellipses in 3D

Distance Between Two Ellipses in 3D Disance Beween Two Ellipses in 3D David Eberly Magic Sofware 6006 Meadow Run Cour Chapel Hill, NC 27516 eberly@magic-sofware.com 1 Inroducion An ellipse in 3D is represened by a cener C, uni lengh axes

More information

arxiv: v1 [math.fa] 19 May 2017

arxiv: v1 [math.fa] 19 May 2017 RELATIVE ENTROPY AND TSALLIS ENTROPY OF TWO ACCRETIVE OPERATORS M. RAÏSSOULI1,2, M. S. MOSLEHIAN 3, AND S. FURUICHI 4 arxiv:175.742v1 [mah.fa] 19 May 217 Absrac. Le A and B be wo accreive operaors. We

More information

Lecture 20: Riccati Equations and Least Squares Feedback Control

Lecture 20: Riccati Equations and Least Squares Feedback Control 34-5 LINEAR SYSTEMS Lecure : Riccai Equaions and Leas Squares Feedback Conrol 5.6.4 Sae Feedback via Riccai Equaions A recursive approach in generaing he marix-valued funcion W ( ) equaion for i for he

More information

Characterization of Gamma Hemirings by Generalized Fuzzy Gamma Ideals

Characterization of Gamma Hemirings by Generalized Fuzzy Gamma Ideals Available a hp://pvamu.edu/aam Appl. Appl. Mah. ISSN: 1932-9466 Vol. 10, Issue 1 (June 2015), pp. 495-520 Applicaions and Applied Mahemaics: An Inernaional Journal (AAM) Characerizaion of Gamma Hemirings

More information

THE MATRIX-TREE THEOREM

THE MATRIX-TREE THEOREM THE MATRIX-TREE THEOREM 1 The Marix-Tree Theorem. The Marix-Tree Theorem is a formula for he number of spanning rees of a graph in erms of he deerminan of a cerain marix. We begin wih he necessary graph-heoreical

More information

10. State Space Methods

10. State Space Methods . Sae Space Mehods. Inroducion Sae space modelling was briefly inroduced in chaper. Here more coverage is provided of sae space mehods before some of heir uses in conrol sysem design are covered in he

More information

The Asymptotic Behavior of Nonoscillatory Solutions of Some Nonlinear Dynamic Equations on Time Scales

The Asymptotic Behavior of Nonoscillatory Solutions of Some Nonlinear Dynamic Equations on Time Scales Advances in Dynamical Sysems and Applicaions. ISSN 0973-5321 Volume 1 Number 1 (2006, pp. 103 112 c Research India Publicaions hp://www.ripublicaion.com/adsa.hm The Asympoic Behavior of Nonoscillaory Soluions

More information

(1) (2) Differentiation of (1) and then substitution of (3) leads to. Therefore, we will simply consider the second-order linear system given by (4)

(1) (2) Differentiation of (1) and then substitution of (3) leads to. Therefore, we will simply consider the second-order linear system given by (4) Phase Plane Analysis of Linear Sysems Adaped from Applied Nonlinear Conrol by Sloine and Li The general form of a linear second-order sysem is a c b d From and b bc d a Differeniaion of and hen subsiuion

More information

SUFFICIENT CONDITIONS FOR EXISTENCE SOLUTION OF LINEAR TWO-POINT BOUNDARY PROBLEM IN MINIMIZATION OF QUADRATIC FUNCTIONAL

SUFFICIENT CONDITIONS FOR EXISTENCE SOLUTION OF LINEAR TWO-POINT BOUNDARY PROBLEM IN MINIMIZATION OF QUADRATIC FUNCTIONAL HE PUBLISHING HOUSE PROCEEDINGS OF HE ROMANIAN ACADEMY, Series A, OF HE ROMANIAN ACADEMY Volume, Number 4/200, pp 287 293 SUFFICIEN CONDIIONS FOR EXISENCE SOLUION OF LINEAR WO-POIN BOUNDARY PROBLEM IN

More information

Representation of Stochastic Process by Means of Stochastic Integrals

Representation of Stochastic Process by Means of Stochastic Integrals Inernaional Journal of Mahemaics Research. ISSN 0976-5840 Volume 5, Number 4 (2013), pp. 385-397 Inernaional Research Publicaion House hp://www.irphouse.com Represenaion of Sochasic Process by Means of

More information

Problem set 6: Solutions Math 207A, Fall x 0 2 x

Problem set 6: Solutions Math 207A, Fall x 0 2 x Problem se 6: Soluions Mah 7A, Fall 14 1 Skech phase planes of he following linear ssems: 4 a = ; 9 4 b = ; 9 1 c = ; 1 d = ; 4 e = ; f = 1 3 In each case, classif he equilibrium, =, as a saddle poin,

More information

FREE ODD PERIODIC ACTIONS ON THE SOLID KLEIN BOTTLE

FREE ODD PERIODIC ACTIONS ON THE SOLID KLEIN BOTTLE An-Najah J. Res. Vol. 1 ( 1989 ) Number 6 Fawas M. Abudiak FREE ODD PERIODIC ACTIONS ON THE SOLID LEIN BOTTLE ey words : Free acion, Periodic acion Solid lein Bole. Fawas M. Abudiak * V.' ZZ..).a11,L.A.;15TY1

More information

Olaru Ion Marian. In 1968, Vasilios A. Staikos [6] studied the equation:

Olaru Ion Marian. In 1968, Vasilios A. Staikos [6] studied the equation: ACTA UNIVERSITATIS APULENSIS No 11/2006 Proceedings of he Inernaional Conference on Theory and Applicaion of Mahemaics and Informaics ICTAMI 2005 - Alba Iulia, Romania THE ASYMPTOTIC EQUIVALENCE OF THE

More information

Improved Approximate Solutions for Nonlinear Evolutions Equations in Mathematical Physics Using the Reduced Differential Transform Method

Improved Approximate Solutions for Nonlinear Evolutions Equations in Mathematical Physics Using the Reduced Differential Transform Method Journal of Applied Mahemaics & Bioinformaics, vol., no., 01, 1-14 ISSN: 179-660 (prin), 179-699 (online) Scienpress Ld, 01 Improved Approimae Soluions for Nonlinear Evoluions Equaions in Mahemaical Physics

More information

arxiv: v1 [math.fa] 9 Dec 2018

arxiv: v1 [math.fa] 9 Dec 2018 AN INVERSE FUNCTION THEOREM CONVERSE arxiv:1812.03561v1 [mah.fa] 9 Dec 2018 JIMMIE LAWSON Absrac. We esablish he following converse of he well-known inverse funcion heorem. Le g : U V and f : V U be inverse

More information

Multi-component Levi Hierarchy and Its Multi-component Integrable Coupling System

Multi-component Levi Hierarchy and Its Multi-component Integrable Coupling System Commun. Theor. Phys. (Beijing, China) 44 (2005) pp. 990 996 c Inernaional Academic Publishers Vol. 44, No. 6, December 5, 2005 uli-componen Levi Hierarchy and Is uli-componen Inegrable Coupling Sysem XIA

More information

A problem related to Bárány Grünbaum conjecture

A problem related to Bárány Grünbaum conjecture Filoma 27:1 (2013), 109 113 DOI 10.2298/FIL1301109B Published by Faculy of Sciences and Mahemaics, Universiy of Niš, Serbia Available a: hp://www.pmf.ni.ac.rs/filoma A problem relaed o Bárány Grünbaum

More information

arxiv: v1 [math.pr] 19 Feb 2011

arxiv: v1 [math.pr] 19 Feb 2011 A NOTE ON FELLER SEMIGROUPS AND RESOLVENTS VADIM KOSTRYKIN, JÜRGEN POTTHOFF, AND ROBERT SCHRADER ABSTRACT. Various equivalen condiions for a semigroup or a resolven generaed by a Markov process o be of

More information

Concourse Math Spring 2012 Worked Examples: Matrix Methods for Solving Systems of 1st Order Linear Differential Equations

Concourse Math Spring 2012 Worked Examples: Matrix Methods for Solving Systems of 1st Order Linear Differential Equations Concourse Mah 80 Spring 0 Worked Examples: Marix Mehods for Solving Sysems of s Order Linear Differenial Equaions The Main Idea: Given a sysem of s order linear differenial equaions d x d Ax wih iniial

More information

Bernoulli numbers. Francesco Chiatti, Matteo Pintonello. December 5, 2016

Bernoulli numbers. Francesco Chiatti, Matteo Pintonello. December 5, 2016 UNIVERSITÁ DEGLI STUDI DI PADOVA, DIPARTIMENTO DI MATEMATICA TULLIO LEVI-CIVITA Bernoulli numbers Francesco Chiai, Maeo Pinonello December 5, 206 During las lessons we have proved he Las Ferma Theorem

More information

Theory of! Partial Differential Equations!

Theory of! Partial Differential Equations! hp://www.nd.edu/~gryggva/cfd-course/! Ouline! Theory o! Parial Dierenial Equaions! Gréar Tryggvason! Spring 011! Basic Properies o PDE!! Quasi-linear Firs Order Equaions! - Characerisics! - Linear and

More information

LAPLACE TRANSFORM AND TRANSFER FUNCTION

LAPLACE TRANSFORM AND TRANSFER FUNCTION CHBE320 LECTURE V LAPLACE TRANSFORM AND TRANSFER FUNCTION Professor Dae Ryook Yang Spring 2018 Dep. of Chemical and Biological Engineering 5-1 Road Map of he Lecure V Laplace Transform and Transfer funcions

More information

On the probabilistic stability of the monomial functional equation

On the probabilistic stability of the monomial functional equation Available online a www.jnsa.com J. Nonlinear Sci. Appl. 6 (013), 51 59 Research Aricle On he probabilisic sabiliy of he monomial funcional equaion Claudia Zaharia Wes Universiy of Timişoara, Deparmen of

More information

Transcendence of solutions of q-airy equation.

Transcendence of solutions of q-airy equation. Josai Mahemaical Monographs vol. 0 (207), pp. 29 37 Transcendence of soluions of q-airy equaion. Seiji NISHIOKA Absrac. In his paper, we prove ranscendence of soluions of he ieraed Riccai equaions associaed

More information

Math From Scratch Lesson 34: Isolating Variables

Math From Scratch Lesson 34: Isolating Variables Mah From Scrach Lesson 34: Isolaing Variables W. Blaine Dowler July 25, 2013 Conens 1 Order of Operaions 1 1.1 Muliplicaion and Addiion..................... 1 1.2 Division and Subracion.......................

More information

( ) ( ) if t = t. It must satisfy the identity. So, bulkiness of the unit impulse (hyper)function is equal to 1. The defining characteristic is

( ) ( ) if t = t. It must satisfy the identity. So, bulkiness of the unit impulse (hyper)function is equal to 1. The defining characteristic is UNIT IMPULSE RESPONSE, UNIT STEP RESPONSE, STABILITY. Uni impulse funcion (Dirac dela funcion, dela funcion) rigorously defined is no sricly a funcion, bu disribuion (or measure), precise reamen requires

More information

Generalized Chebyshev polynomials

Generalized Chebyshev polynomials Generalized Chebyshev polynomials Clemene Cesarano Faculy of Engineering, Inernaional Telemaic Universiy UNINETTUNO Corso Viorio Emanuele II, 39 86 Roma, Ialy email: c.cesarano@unineunouniversiy.ne ABSTRACT

More information

DISCRETE GRONWALL LEMMA AND APPLICATIONS

DISCRETE GRONWALL LEMMA AND APPLICATIONS DISCRETE GRONWALL LEMMA AND APPLICATIONS JOHN M. HOLTE MAA NORTH CENTRAL SECTION MEETING AT UND 24 OCTOBER 29 Gronwall s lemma saes an inequaliy ha is useful in he heory of differenial equaions. Here is

More information

Essential Maps and Coincidence Principles for General Classes of Maps

Essential Maps and Coincidence Principles for General Classes of Maps Filoma 31:11 (2017), 3553 3558 hps://doi.org/10.2298/fil1711553o Published by Faculy of Sciences Mahemaics, Universiy of Niš, Serbia Available a: hp://www.pmf.ni.ac.rs/filoma Essenial Maps Coincidence

More information

NEW EXAMPLES OF CONVOLUTIONS AND NON-COMMUTATIVE CENTRAL LIMIT THEOREMS

NEW EXAMPLES OF CONVOLUTIONS AND NON-COMMUTATIVE CENTRAL LIMIT THEOREMS QUANTUM PROBABILITY BANACH CENTER PUBLICATIONS, VOLUME 43 INSTITUTE OF MATHEMATICS POLISH ACADEMY OF SCIENCES WARSZAWA 998 NEW EXAMPLES OF CONVOLUTIONS AND NON-COMMUTATIVE CENTRAL LIMIT THEOREMS MAREK

More information

Theory of! Partial Differential Equations-I!

Theory of! Partial Differential Equations-I! hp://users.wpi.edu/~grear/me61.hml! Ouline! Theory o! Parial Dierenial Equaions-I! Gréar Tryggvason! Spring 010! Basic Properies o PDE!! Quasi-linear Firs Order Equaions! - Characerisics! - Linear and

More information

Orthogonal Rational Functions, Associated Rational Functions And Functions Of The Second Kind

Orthogonal Rational Functions, Associated Rational Functions And Functions Of The Second Kind Proceedings of he World Congress on Engineering 2008 Vol II Orhogonal Raional Funcions, Associaed Raional Funcions And Funcions Of The Second Kind Karl Deckers and Adhemar Bulheel Absrac Consider he sequence

More information

t j i, and then can be naturally extended to K(cf. [S-V]). The Hasse derivatives satisfy the following: is defined on k(t) by D (i)

t j i, and then can be naturally extended to K(cf. [S-V]). The Hasse derivatives satisfy the following: is defined on k(t) by D (i) A NOTE ON WRONSKIANS AND THE ABC THEOREM IN FUNCTION FIELDS OF RIME CHARACTERISTIC Julie Tzu-Yueh Wang Insiue of Mahemaics Academia Sinica Nankang, Taipei 11529 Taiwan, R.O.C. May 14, 1998 Absrac. We provide

More information

CERTAIN CLASSES OF SOLUTIONS OF LAGERSTROM EQUATIONS

CERTAIN CLASSES OF SOLUTIONS OF LAGERSTROM EQUATIONS SARAJEVO JOURNAL OF MATHEMATICS Vol.10 (22 (2014, 67 76 DOI: 10.5644/SJM.10.1.09 CERTAIN CLASSES OF SOLUTIONS OF LAGERSTROM EQUATIONS ALMA OMERSPAHIĆ AND VAHIDIN HADŽIABDIĆ Absrac. This paper presens sufficien

More information

Generalized Snell envelope and BSDE With Two general Reflecting Barriers

Generalized Snell envelope and BSDE With Two general Reflecting Barriers 1/22 Generalized Snell envelope and BSDE Wih Two general Reflecing Barriers EL HASSAN ESSAKY Cadi ayyad Universiy Poly-disciplinary Faculy Safi Work in progress wih : M. Hassani and Y. Ouknine Iasi, July

More information

A Necessary and Sufficient Condition for the Solutions of a Functional Differential Equation to Be Oscillatory or Tend to Zero

A Necessary and Sufficient Condition for the Solutions of a Functional Differential Equation to Be Oscillatory or Tend to Zero JOURNAL OF MAEMAICAL ANALYSIS AND APPLICAIONS 24, 7887 1997 ARICLE NO. AY965143 A Necessary and Sufficien Condiion for he Soluions of a Funcional Differenial Equaion o Be Oscillaory or end o Zero Piambar

More information

arxiv: v6 [math-ph] 24 Dec 2016

arxiv: v6 [math-ph] 24 Dec 2016 A REFORMULATION OF THE GENERALIZED q-painlevé VI SYSTEM WITH W(A () 2n+ ) SYMMETRY TAKAO SUZUKI arxiv:6020573v6 [mah-ph] 24 Dec 206 Absrac In he previous work we inroduced he higher order q-painlevé sysem

More information

The motions of the celt on a horizontal plane with viscous friction

The motions of the celt on a horizontal plane with viscous friction The h Join Inernaional Conference on Mulibody Sysem Dynamics June 8, 18, Lisboa, Porugal The moions of he cel on a horizonal plane wih viscous fricion Maria A. Munisyna 1 1 Moscow Insiue of Physics and

More information

Solitons Solutions to Nonlinear Partial Differential Equations by the Tanh Method

Solitons Solutions to Nonlinear Partial Differential Equations by the Tanh Method IOSR Journal of Mahemaics (IOSR-JM) e-issn: 7-7,p-ISSN: 319-7X, Volume, Issue (Sep. - Oc. 13), PP 1-19 Solions Soluions o Nonlinear Parial Differenial Equaions by he Tanh Mehod YusurSuhail Ali Compuer

More information

Ann. Funct. Anal. 2 (2011), no. 2, A nnals of F unctional A nalysis ISSN: (electronic) URL:

Ann. Funct. Anal. 2 (2011), no. 2, A nnals of F unctional A nalysis ISSN: (electronic) URL: Ann. Func. Anal. 2 2011, no. 2, 34 41 A nnals of F uncional A nalysis ISSN: 2008-8752 elecronic URL: www.emis.de/journals/afa/ CLASSIFICAION OF POSIIVE SOLUIONS OF NONLINEAR SYSEMS OF VOLERRA INEGRAL EQUAIONS

More information

Asymptotic instability of nonlinear differential equations

Asymptotic instability of nonlinear differential equations Elecronic Journal of Differenial Equaions, Vol. 1997(1997), No. 16, pp. 1 7. ISSN: 172-6691. URL: hp://ejde.mah.sw.edu or hp://ejde.mah.un.edu fp (login: fp) 147.26.13.11 or 129.12.3.113 Asympoic insabiliy

More information

Cash Flow Valuation Mode Lin Discrete Time

Cash Flow Valuation Mode Lin Discrete Time IOSR Journal of Mahemaics (IOSR-JM) e-issn: 2278-5728,p-ISSN: 2319-765X, 6, Issue 6 (May. - Jun. 2013), PP 35-41 Cash Flow Valuaion Mode Lin Discree Time Olayiwola. M. A. and Oni, N. O. Deparmen of Mahemaics

More information

Finish reading Chapter 2 of Spivak, rereading earlier sections as necessary. handout and fill in some missing details!

Finish reading Chapter 2 of Spivak, rereading earlier sections as necessary. handout and fill in some missing details! MAT 257, Handou 6: Ocober 7-2, 20. I. Assignmen. Finish reading Chaper 2 of Spiva, rereading earlier secions as necessary. handou and fill in some missing deails! II. Higher derivaives. Also, read his

More information

Fuzzy Laplace Transforms for Derivatives of Higher Orders

Fuzzy Laplace Transforms for Derivatives of Higher Orders Maemaical Teory and Modeling ISSN -58 (Paper) ISSN 5-5 (Online) Vol, No, 1 wwwiiseorg Fuzzy Laplace Transforms for Derivaives of Higer Orders Absrac Amal K Haydar 1 *and Hawrra F Moammad Ali 1 College

More information

A NOTE ON THE STRUCTURE OF BILATTICES. A. Avron. School of Mathematical Sciences. Sackler Faculty of Exact Sciences. Tel Aviv University

A NOTE ON THE STRUCTURE OF BILATTICES. A. Avron. School of Mathematical Sciences. Sackler Faculty of Exact Sciences. Tel Aviv University A NOTE ON THE STRUCTURE OF BILATTICES A. Avron School of Mahemaical Sciences Sacler Faculy of Exac Sciences Tel Aviv Universiy Tel Aviv 69978, Israel The noion of a bilaice was rs inroduced by Ginsburg

More information

Math 10B: Mock Mid II. April 13, 2016

Math 10B: Mock Mid II. April 13, 2016 Name: Soluions Mah 10B: Mock Mid II April 13, 016 1. ( poins) Sae, wih jusificaion, wheher he following saemens are rue or false. (a) If a 3 3 marix A saisfies A 3 A = 0, hen i canno be inverible. True.

More information

The Fine Structure of LD-Equivalence

The Fine Structure of LD-Equivalence Advances in Mahemaics 155, 264316 (2000) doi:10.1006aima.2000.1938, available online a hp:www.idealibrary.com on The Fine Srucure of LD-Equivalence Parick Dehornoy Mahe maiques, laboraoire SDAD, ESA 6081

More information

Conservation laws of a perturbed Kaup Newell equation

Conservation laws of a perturbed Kaup Newell equation Modern Physics Leers B Vol. 30, Nos. 32 & 33 (2016) 1650381 (6 pages) c World Scienific Publishing Company DOI: 10.1142/S0217984916503814 Conservaion laws of a perurbed Kaup Newell equaion Jing-Yun Yang

More information

Application of He s Variational Iteration Method for Solving Seventh Order Sawada-Kotera Equations

Application of He s Variational Iteration Method for Solving Seventh Order Sawada-Kotera Equations Applied Mahemaical Sciences, Vol. 2, 28, no. 1, 471-477 Applicaion of He s Variaional Ieraion Mehod for Solving Sevenh Order Sawada-Koera Equaions Hossein Jafari a,1, Allahbakhsh Yazdani a, Javad Vahidi

More information

MATH 128A, SUMMER 2009, FINAL EXAM SOLUTION

MATH 128A, SUMMER 2009, FINAL EXAM SOLUTION MATH 28A, SUMME 2009, FINAL EXAM SOLUTION BENJAMIN JOHNSON () (8 poins) [Lagrange Inerpolaion] (a) (4 poins) Le f be a funcion defined a some real numbers x 0,..., x n. Give a defining equaion for he Lagrange

More information

Integral representations and new generating functions of Chebyshev polynomials

Integral representations and new generating functions of Chebyshev polynomials Inegral represenaions an new generaing funcions of Chebyshev polynomials Clemene Cesarano Faculy of Engineering, Inernaional Telemaic Universiy UNINETTUNO Corso Viorio Emanuele II, 39 186 Roma, Ialy email:

More information

Convergence of the Neumann series in higher norms

Convergence of the Neumann series in higher norms Convergence of he Neumann series in higher norms Charles L. Epsein Deparmen of Mahemaics, Universiy of Pennsylvania Version 1.0 Augus 1, 003 Absrac Naural condiions on an operaor A are given so ha he Neumann

More information

On Carlsson type orthogonality and characterization of inner product spaces

On Carlsson type orthogonality and characterization of inner product spaces Filoma 26:4 (212), 859 87 DOI 1.2298/FIL124859K Published by Faculy of Sciences and Mahemaics, Universiy of Niš, Serbia Available a: hp://www.pmf.ni.ac.rs/filoma On Carlsson ype orhogonaliy and characerizaion

More information

ON UNIVERSAL LOCALIZATION AT SEMIPRIME GOLDIE IDEALS

ON UNIVERSAL LOCALIZATION AT SEMIPRIME GOLDIE IDEALS ON UNIVERSAL LOCALIZATION AT SEMIPRIME GOLDIE IDEALS JOHN A. BEACHY Deparmen of Mahemaical Sciences Norhern Illinois Universiy DeKalb IL 6115 U.S.A. Absrac In his paper we consider an alernaive o Ore localizaion

More information

Math 334 Fall 2011 Homework 11 Solutions

Math 334 Fall 2011 Homework 11 Solutions Dec. 2, 2 Mah 334 Fall 2 Homework Soluions Basic Problem. Transform he following iniial value problem ino an iniial value problem for a sysem: u + p()u + q() u g(), u() u, u () v. () Soluion. Le v u. Then

More information

CHAPTER 2: Mathematics for Microeconomics

CHAPTER 2: Mathematics for Microeconomics CHAPTER : Mahemaics for Microeconomics The problems in his chaper are primarily mahemaical. They are inended o give sudens some pracice wih he conceps inroduced in Chaper, bu he problems in hemselves offer

More information

Differential Harnack Estimates for Parabolic Equations

Differential Harnack Estimates for Parabolic Equations Differenial Harnack Esimaes for Parabolic Equaions Xiaodong Cao and Zhou Zhang Absrac Le M,g be a soluion o he Ricci flow on a closed Riemannian manifold In his paper, we prove differenial Harnack inequaliies

More information

A remark on the H -calculus

A remark on the H -calculus A remark on he H -calculus Nigel J. Kalon Absrac If A, B are secorial operaors on a Hilber space wih he same domain range, if Ax Bx A 1 x B 1 x, hen i is a resul of Auscher, McInosh Nahmod ha if A has

More information

d 1 = c 1 b 2 - b 1 c 2 d 2 = c 1 b 3 - b 1 c 3

d 1 = c 1 b 2 - b 1 c 2 d 2 = c 1 b 3 - b 1 c 3 and d = c b - b c c d = c b - b c c This process is coninued unil he nh row has been compleed. The complee array of coefficiens is riangular. Noe ha in developing he array an enire row may be divided or

More information

New effective moduli of isotropic viscoelastic composites. Part I. Theoretical justification

New effective moduli of isotropic viscoelastic composites. Part I. Theoretical justification IOP Conference Series: Maerials Science and Engineering PAPE OPEN ACCESS New effecive moduli of isoropic viscoelasic composies. Par I. Theoreical jusificaion To cie his aricle: A A Sveashkov and A A akurov

More information

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

dt = C exp (3 ln t 4 ). t 4 W = C exp ( ln(4 t) 3) = C(4 t) 3. Mah Rahman Exam Review Soluions () Consider he IVP: ( 4)y 3y + 4y = ; y(3) = 0, y (3) =. (a) Please deermine he longes inerval for which he IVP is guaraneed o have a unique soluion. Soluion: The disconinuiies

More information

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

Solutions of Sample Problems for Third In-Class Exam Math 246, Spring 2011, Professor David Levermore Soluions of Sample Problems for Third In-Class Exam Mah 6, Spring, Professor David Levermore Compue he Laplace ransform of f e from is definiion Soluion The definiion of he Laplace ransform gives L[f]s

More information

The expectation value of the field operator.

The expectation value of the field operator. The expecaion value of he field operaor. Dan Solomon Universiy of Illinois Chicago, IL dsolom@uic.edu June, 04 Absrac. Much of he mahemaical developmen of quanum field heory has been in suppor of deermining

More information

MATH 2050 Assignment 9 Winter Do not need to hand in. 1. Find the determinant by reducing to triangular form for the following matrices.

MATH 2050 Assignment 9 Winter Do not need to hand in. 1. Find the determinant by reducing to triangular form for the following matrices. MATH 2050 Assignmen 9 Winer 206 Do no need o hand in Noe ha he final exam also covers maerial afer HW8, including, for insance, calculaing deerminan by row operaions, eigenvalues and eigenvecors, similariy

More information

STABILITY OF NONLINEAR NEUTRAL DELAY DIFFERENTIAL EQUATIONS WITH VARIABLE DELAYS

STABILITY OF NONLINEAR NEUTRAL DELAY DIFFERENTIAL EQUATIONS WITH VARIABLE DELAYS Elecronic Journal of Differenial Equaions, Vol. 217 217, No. 118, pp. 1 14. ISSN: 172-6691. URL: hp://ejde.mah.xsae.edu or hp://ejde.mah.un.edu STABILITY OF NONLINEAR NEUTRAL DELAY DIFFERENTIAL EQUATIONS

More information

Ordinary Differential Equations

Ordinary Differential Equations Ordinary Differenial Equaions 5. Examples of linear differenial equaions and heir applicaions We consider some examples of sysems of linear differenial equaions wih consan coefficiens y = a y +... + a

More information

18 Biological models with discrete time

18 Biological models with discrete time 8 Biological models wih discree ime The mos imporan applicaions, however, may be pedagogical. The elegan body of mahemaical heory peraining o linear sysems (Fourier analysis, orhogonal funcions, and so

More information

Differential Equations

Differential Equations Mah 21 (Fall 29) Differenial Equaions Soluion #3 1. Find he paricular soluion of he following differenial equaion by variaion of parameer (a) y + y = csc (b) 2 y + y y = ln, > Soluion: (a) The corresponding

More information

The Eigenvalue Problems - 8.8

The Eigenvalue Problems - 8.8 The Eigenvalue Problems - 8.8. Definiion of Eigenvalues and Eigenvecors: Le A be an n! n marix. A scalar s said o be an eigenvalue of A if he linear sysem Av!v has a nonzero soluion vecor v. The soluion

More information

A natural selection of a graphic contraction transformation in fuzzy metric spaces

A natural selection of a graphic contraction transformation in fuzzy metric spaces Available online a www.isr-publicaions.com/jnsa J. Nonlinear Sci. Appl., (208), 28 227 Research Aricle Journal Homepage: www.isr-publicaions.com/jnsa A naural selecion of a graphic conracion ransformaion

More information

Math Week 14 April 16-20: sections first order systems of linear differential equations; 7.4 mass-spring systems.

Math Week 14 April 16-20: sections first order systems of linear differential equations; 7.4 mass-spring systems. Mah 2250-004 Week 4 April 6-20 secions 7.-7.3 firs order sysems of linear differenial equaions; 7.4 mass-spring sysems. Mon Apr 6 7.-7.2 Sysems of differenial equaions (7.), and he vecor Calculus we need

More information