Variational analysis of some questions in dynamical system and biological system

Size: px
Start display at page:

Download "Variational analysis of some questions in dynamical system and biological system"

Transcription

1 Available online Journal of Chemical an Pharmaceutical Research, 014, 6(7): Research Article ISSN : CODEN(USA) : JCPRC5 Variational analsis of some questions in namical sstem an biological sstem Sun Dawei an Liu Jiarui College of Science, Henan Universit an Technolog, Zhengzhou, China ABSTRACT This paper stuies the variational problems of some namical sstem. B using the methos of Euler equation an Legenre conitions an some computional techniques in mechanics an ifferential equations, this paper computes the extrema of some sstems an iscuss some future applications in smplectic namical sstems an biological mathematical problems. Ke wors: variational methos; Euler equation; biological mathematical problems INTRODUCTION Variational methos pla an important role in mathematics, mechanics an other science an technologies. In the earl 16 centur, Newton, Leibnitz, Euler, Lagrange an other scientists have stuie the variational methos [1]. The origin of the variational methos is the problem of brachistochrone curve, which carries a point-like bo from one place to another in the least amount of time. Newton, Leibnitz an Johann Bernoulli solve this problem an their methos give the iea of variational methos. Another problem is the geoesic problem; it is fining the shortest path connecting two points. On a Riemannian manifol M with riemannian metric g, the length of a smooth curve γ : [a,b] M is efine b the following: L( γ) = g (& γ, & γ ) γ (1) The minimizing curves of L in a small enough open set can be obtaine b techniques of calculus of variations. The existence an uniqueness problem of geoesics promote the evelopment of geometr. Variational methos have man important applications in ifferential equations. Solving a ifferential equation is the same with fining the critical points of some variational functional. This iea was first use in the ifferential equation of secon orer. For example we see the next bounar value prblem of linear elliptic equation [,3] u = f (x), x Ω u = 0, x Ω Here Ω is boune omain with smooth bounar of the Eucil space. B variational metho, one can translate this problem to be fining the critical points of the functional: 1 I (v) = ( Dv fv) Ω (3) The process of fining the critical points of this functional is to fin the extremal point of tihs functional. Later, () 184

2 peple use the lower semi-continuit conition to stu the egenerate elliptic problem: p u ( u) = f, in Ω u = 0, x Ω (4) The ke point to solve this elliptic problem is fining the extremal point of its corresponing functional. B the usual classic result,we have if M is topological Hausorff space, an suppose that a functional satisfies the conition of boune compactness(heine-borel propert), then E is uniforml boune from below an attain its infimum on M. However, the conition of boune compactness is not eas to confirme, so people tr to use some facts that can be checke easil to instea the above classical results. Suppose V is a reflexive banach space with norm, an M V is a weakl close subset of V. Suppose that a functional E is coercive an weak lower semi-continuous on M with respect to V. Then the functional E is boune from below on M an attains its infimum in M. Using the moifie results, one can check that the corresponing functional : 1 p E(u) = u fu p Ω Ω (5) 1, P W0 ( Ω) is reflexive an Satisfies the requirment of the moifie facts. It is eas to checke that the banach space the the functional is coercive an weak sequentiall lower semi-continuous. So the above results implies that there is a minimizer for the functional, an therefore there is a solution for the egenerate elliptic problem. In general people can not get that a boune an lower semi-continuous functional get its infimum. Ekelan construct minimizing sequence an show that there exists nearl optimal solutions to some optimization problems. An this principle can be use when the level set is not compact. Compactness becomes more an more important. To overcome this ifficult of lacking compactness, Palis an Smale introuce the concepts of PS-conition: a sequence u m in V is calle a Palais-Smale sequence for E if of the functional Palais-Smale sequence has a convergent subsequence. E (u ) m c uniforml in m, while the Differential DE(u m) 0 as m 0, a functional E is sai to satisf the Palais-Smale conition if an In 1970s, A.Ambrosetti an P.Rabinowitz use the Mountain pass theorem to solve some ifferential equations[6]. P.Rabinowitz prove the perioic solutions of the Hamiltonian sstem. Later Benci-Rabinowitz give the linking argument, the can solve more semilinear elliptic bounar problem without smmetr. There are other evelopments for the variational methos, an the applications in smplectic geometr an namical sstem, we will iscuss later. In this paper, we will first introuce some basic notions of variational methos, show the basic techniques to fin the extrema, an give some example to reall fin the extrema, an last we show the applicaition in smplectic geometr an iscuss some future the variational methos mabe ca be use. 1. PREPARATIONS AND LEMMAS.1 Preparations In this section, we briefl introuce the notations of variational methos; give some basic lemmas an properties of Euler equations, Jacobi conitions an some variational problems for geometr, for etails we refer to [1,, 3, 4, 7]. Definition 1 A function f n is lower semi continuous at a point x if the following ientities hol: liminf f (x) = f ( x) x x (6) The lower semi continuous is equivalent as the following [13]: Theorem. The following properties of a function f are equivalent 185

3 1. F is lower semicontinuous. The epigraph set is close 3. The level set are close. Definition 3. Fréchet erivative of a function is efine as following: Let V an W be Banach spaces, an U V be an open subset of V. A function f: U W is calle Fréchet ifferentiable at x U if there exists a boune linear operator AX : V W such that f (x+ h) f(x) A x (h) w lim = 0 h 0 h v (7) Now we give the funamental theorem of calculus of calculus of variations. Definition 4 If a function Ω u(x) f(x) = 0, f ( Ω) Then 0 C 0 u C( Ω) satisfies [1] u = in Ω.Next we introuce the Euler equation of the variational functional [1]: Lemma 5 If the functional ' [(x)] (x,, ) = J F (8) (9) Satisfies the bounar value conitions (x ), (x ) = = Then the extremal curve shoul satisf the following equation F F = 0 ' (10) Here the function F is of secon orer. An this equation is also calle Euler- Lagrange equation. This equation can also be written as the following F F F ' F '' ' ' x = 0 Once we have the Euler- Lagrange equation, we can translate the extrmal problem to solve ifferential equations.if there are more variables, the Euler- Lagrange equation can also be foun. (11) Lemma 6 If the functional ' ' [(x),z(x)] (x,, z, z ) = J F get its extrema an satisfies the bounar value conitions (x ) =, (x ) =,z(x ) = z,z(x ) = z Then there extremal curve satisfies the following Euler- Lagrange equations F F F = F = 0 ' z z ' 0 (1) (13) (14) 186

4 If the variational functional has man variables, the Euler- Lagrange equations can also be written in the same wa. Moreover, if the functional epen on the higher orer ifferential of the variables, ' '' [(x)] (x,,, ) = J F (15) Suppose that this functional gets its extrema an satisfies the bounar value conition (x ) =, (x ) =, '(x ) = ', '(x ) = ' (16) Here the variational functional shoul be ifferential of thir orer, the function is ifferential of fourth orer, then the Euler- Lagrange equation is as following: F F F + = ' '' 0 This equation is also calle Euler-Poisson equation. If there are more variables, the Euler-Poisson equation can also be extene to that case, just note that the functional an the function shoul have higher ifferentiation [1]. (17) Next we introuce some sufficient conitions of extrema of Functionals. Consier the functional ' [(x)] (x,, ) = J F With the bounar value conition (x ) =, (x ) = If the functional attains its extrema at u(x), then we have the following equation u ( F F ') u ( F ' ' ) = 0 (18) (19) (0) This equation is calle the Jacobi equation. It is the same with fining the extrema of functions with one variable; we nee some sufficient conitions to etermine whether a functional can get its extrema. This is the classical Weiestrass sufficient conitions an Legenre Sufficient conitions. Let E(x,, ', p) = F(x,, ') F(x,, p) (' p) F (x,,p) p (1) Theorem 7. If the function =(x) is the extremal curve of the functional an satisfies the bounar value conition, ' an also satisfies the Jacobi conitions, for all near, the Weiestrass conitions hol,we get its local infmum, if it is less than zero, we get its local Maxima.. Example Now we give some examples to show how to etermine the extrema. Example 8. Fin the extremal curve of the following functional π 4 J (, z) = 3z 9 + ' z ' 0 The bounar conitions are: (0) = 0, ( π ) =, z(0) = 0, z( π ) = π B the Euler- Lagrange equations, we can compute that the function F is F(, z) = 3z 9 + ' z ' () (3) (4) 187

5 So we can compute the z ' z ' F, F, F, F, so the Euler- Lagrange equations are the following ifferential equations: 18 + '' = z '' = 0 (5) Integral the equations, we can get the solutions of this equations are cos3 sin 3 = c1 x + c x 3 z = x + c3x + c4 8 Accoring to the bounar conitions, we can get that 3 + 3π c1 = 0, c4 = 0, c =, c3 = 3 So the extremal curve is = sin 3x π z = x + x 8 3 (6) (7) (8) Next we see the applications of the Jacobi equations, an we just give the iea of the compute an omit the result. Example 9. Suppose that the functional is the following J () = ( x ' ) (x 0) = 0, (x 1) = 1 (9) Fin the solution whose Jacobi equation satisfies the initial bounar conitions: u (0) = 0, u'(0) = 1 First, we can fin the function F (x,, ') = x ' An we can compute the Euler equation, then b the efinition of Jacobi equation u ( F F ') u ( F ' ' ) = 0 (30) (31) (3) We can get 6u 4 u '' = 0 (33) The solution is u(x) = 1 e + e 1.5x 1.5x An b the initial value of u, we can compute the number 1,, we omit the process. (34) Next we give some other applications of variational methos in smplectic geometr an other namical sstems. First we introuce the bi-invariant metric on the group of Hamiltonian iffeomorphisms. A manifol is smplectic if it is a smooth manifol an equippe with a close non-egenerate ifferential -form, the Hamiltonian iffeomorphism is the time-1 map of the following namical sstem 188

6 ( f& t ) ω Ft i = Hofer first efine a bi-invariant metric on the group of compactl supporte smplectic iffeomorphisms of stanar smplectic manifol [5], the Hofer norm is efine as following. E ( ϕ ) inf{ f f = ϕ} = t 1 f t (36) Viterbo also efine an invariant istance b generating functions an Polterovich evelope this metric on more smplectic manifol [11, 1], finall Lalone an McDuff extene it to an smplectic manifol [10]. In the efinition an proof of Hofer, an Infinite imensional variational metho was use for the variational functional of the Hamiltonian sstem. An interesting question is whether there exist some more variational results for the geoesic problem uner the Hofer metric. How about the variational analsis on the contact bi-invariant metric? Are the similar results for the geoesic problem? Secon we will iscuss some applications of variational methos in the biological sstem. One tpical moel is the equations for two tpes of living creatures live in one foo source. The moles are the following[8,9] S ' = D(1 + be(t) S) m x s m x s a + S a + S x s x ' = m D x a1 + S x s x ' = m D x a + S (39) Here x is the number of the living creature, s is the concentration of nutrient solution, mis the rate of growing. Smith use the variational theorems to stu this problem an analsis the changes of the iving creatures. An this methos can also be use for the analsis of insets in the cereals. CONCLUSION In this paper we introuce the histor an some techniques in variational methos. We compute some extremas of functional b the Euler equation an the Jacobi equation, an iscuss some future applications in smplectic namical sstems an biological mathematical problems Acknowlegments The author woul like to thank the support of Henan Universit of Technolog, uner which the present work was possible. REFERENCES [1] Dazhong Lao. Funamentals of the calculus of variations. Beijing: National Defence Inustr Press, 011. (In chinese). [] Benjin Xuan. Variational methos: theor an applications. Hefui: Press of Universit of Science an Technolog of China, 006. [3] Struwe. M. Variational methos applications to nonlinear partial ifferential equations an Hamiltonian sstem, springer-verlag, [4] Willem.M. Minimax theorems. Progress in Nonlinear ifferential equations an their applications, Birkhauser, [5] Hofer. H, Zehner.E. Smplectic Invariants an Hamiltonian Dnamics. Birkhauser,1994 [6] Ambrosetti A., Rabinowitz. P. Dual variational methos in critical point theor an applications. J.Func.anal.14(1973), [7] Wenrui, Lu. Variational methos in ifferential equations, Beijing, Science press,003. (In chinese) [8] Qizhi L, Jing L. Theoretical stu of mathematical moels of competition, Beijing, Science press,003.(in chinese) [9] Smith H. L. Competitive coexistence in an oscillationg chemostat, SIAM J. Appl. Math. 40:498-5,1981. (35) (37) (38) 189

7 [10] Lalone F, McDuff D.: The Geometr of Smplectic Energ. Ann. Math.141, [11] Viterbo C. Smplectic topolog as the geometr of generating functions. Math. Annalen. Vol 9, Issue 1, pp , 199, [1] Polterovich L. The geometr of the Group of Smplectic Diffeomorphism. Berlin: Birkhauser,001 [13] Rockafellar R, Wets R. Variational analsis Springer,

CHAPTER 1 : DIFFERENTIABLE MANIFOLDS. 1.1 The definition of a differentiable manifold

CHAPTER 1 : DIFFERENTIABLE MANIFOLDS. 1.1 The definition of a differentiable manifold CHAPTER 1 : DIFFERENTIABLE MANIFOLDS 1.1 The efinition of a ifferentiable manifol Let M be a topological space. This means that we have a family Ω of open sets efine on M. These satisfy (1), M Ω (2) the

More information

Darboux s theorem and symplectic geometry

Darboux s theorem and symplectic geometry Darboux s theorem an symplectic geometry Liang, Feng May 9, 2014 Abstract Symplectic geometry is a very important branch of ifferential geometry, it is a special case of poisson geometry, an coul also

More information

6 General properties of an autonomous system of two first order ODE

6 General properties of an autonomous system of two first order ODE 6 General properties of an autonomous system of two first orer ODE Here we embark on stuying the autonomous system of two first orer ifferential equations of the form ẋ 1 = f 1 (, x 2 ), ẋ 2 = f 2 (, x

More information

1 M3-4-5A16 Assessed Problems # 1: Do 4 out of 5 problems

1 M3-4-5A16 Assessed Problems # 1: Do 4 out of 5 problems D. D. Holm M3-4-5A16 Assesse Problems # 1 Due 1 Nov 2012 1 1 M3-4-5A16 Assesse Problems # 1: Do 4 out of 5 problems Exercise 1.1 (Poisson brackets for the Hopf map) Figure 1: The Hopf map. In coorinates

More information

II. First variation of functionals

II. First variation of functionals II. First variation of functionals The erivative of a function being zero is a necessary conition for the etremum of that function in orinary calculus. Let us now tackle the question of the equivalent

More information

Computing Exact Confidence Coefficients of Simultaneous Confidence Intervals for Multinomial Proportions and their Functions

Computing Exact Confidence Coefficients of Simultaneous Confidence Intervals for Multinomial Proportions and their Functions Working Paper 2013:5 Department of Statistics Computing Exact Confience Coefficients of Simultaneous Confience Intervals for Multinomial Proportions an their Functions Shaobo Jin Working Paper 2013:5

More information

Euler equations for multiple integrals

Euler equations for multiple integrals Euler equations for multiple integrals January 22, 2013 Contents 1 Reminer of multivariable calculus 2 1.1 Vector ifferentiation......................... 2 1.2 Matrix ifferentiation........................

More information

Lie symmetry and Mei conservation law of continuum system

Lie symmetry and Mei conservation law of continuum system Chin. Phys. B Vol. 20, No. 2 20 020 Lie symmetry an Mei conservation law of continuum system Shi Shen-Yang an Fu Jing-Li Department of Physics, Zhejiang Sci-Tech University, Hangzhou 3008, China Receive

More information

JUST THE MATHS UNIT NUMBER DIFFERENTIATION 2 (Rates of change) A.J.Hobson

JUST THE MATHS UNIT NUMBER DIFFERENTIATION 2 (Rates of change) A.J.Hobson JUST THE MATHS UNIT NUMBER 10.2 DIFFERENTIATION 2 (Rates of change) by A.J.Hobson 10.2.1 Introuction 10.2.2 Average rates of change 10.2.3 Instantaneous rates of change 10.2.4 Derivatives 10.2.5 Exercises

More information

A Note on Exact Solutions to Linear Differential Equations by the Matrix Exponential

A Note on Exact Solutions to Linear Differential Equations by the Matrix Exponential Avances in Applie Mathematics an Mechanics Av. Appl. Math. Mech. Vol. 1 No. 4 pp. 573-580 DOI: 10.4208/aamm.09-m0946 August 2009 A Note on Exact Solutions to Linear Differential Equations by the Matrix

More information

Agmon Kolmogorov Inequalities on l 2 (Z d )

Agmon Kolmogorov Inequalities on l 2 (Z d ) Journal of Mathematics Research; Vol. 6, No. ; 04 ISSN 96-9795 E-ISSN 96-9809 Publishe by Canaian Center of Science an Eucation Agmon Kolmogorov Inequalities on l (Z ) Arman Sahovic Mathematics Department,

More information

Table of Common Derivatives By David Abraham

Table of Common Derivatives By David Abraham Prouct an Quotient Rules: Table of Common Derivatives By Davi Abraham [ f ( g( ] = [ f ( ] g( + f ( [ g( ] f ( = g( [ f ( ] g( g( f ( [ g( ] Trigonometric Functions: sin( = cos( cos( = sin( tan( = sec

More information

Lectures - Week 10 Introduction to Ordinary Differential Equations (ODES) First Order Linear ODEs

Lectures - Week 10 Introduction to Ordinary Differential Equations (ODES) First Order Linear ODEs Lectures - Week 10 Introuction to Orinary Differential Equations (ODES) First Orer Linear ODEs When stuying ODEs we are consiering functions of one inepenent variable, e.g., f(x), where x is the inepenent

More information

Problem set 2: Solutions Math 207B, Winter 2016

Problem set 2: Solutions Math 207B, Winter 2016 Problem set : Solutions Math 07B, Winter 016 1. A particle of mass m with position x(t) at time t has potential energy V ( x) an kinetic energy T = 1 m x t. The action of the particle over times t t 1

More information

Implicit Differentiation

Implicit Differentiation Implicit Differentiation Thus far, the functions we have been concerne with have been efine explicitly. A function is efine explicitly if the output is given irectly in terms of the input. For instance,

More information

A new proof of the sharpness of the phase transition for Bernoulli percolation on Z d

A new proof of the sharpness of the phase transition for Bernoulli percolation on Z d A new proof of the sharpness of the phase transition for Bernoulli percolation on Z Hugo Duminil-Copin an Vincent Tassion October 8, 205 Abstract We provie a new proof of the sharpness of the phase transition

More information

Lagrangian and Hamiltonian Mechanics

Lagrangian and Hamiltonian Mechanics Lagrangian an Hamiltonian Mechanics.G. Simpson, Ph.. epartment of Physical Sciences an Engineering Prince George s Community College ecember 5, 007 Introuction In this course we have been stuying classical

More information

PDE Notes, Lecture #11

PDE Notes, Lecture #11 PDE Notes, Lecture # from Professor Jalal Shatah s Lectures Febuary 9th, 2009 Sobolev Spaces Recall that for u L loc we can efine the weak erivative Du by Du, φ := udφ φ C0 If v L loc such that Du, φ =

More information

The derivative of a function f(x) is another function, defined in terms of a limiting expression: f(x + δx) f(x)

The derivative of a function f(x) is another function, defined in terms of a limiting expression: f(x + δx) f(x) Y. D. Chong (2016) MH2801: Complex Methos for the Sciences 1. Derivatives The erivative of a function f(x) is another function, efine in terms of a limiting expression: f (x) f (x) lim x δx 0 f(x + δx)

More information

Calculus and optimization

Calculus and optimization Calculus an optimization These notes essentially correspon to mathematical appenix 2 in the text. 1 Functions of a single variable Now that we have e ne functions we turn our attention to calculus. A function

More information

Equations of lines in

Equations of lines in Roberto s Notes on Linear Algebra Chapter 6: Lines, planes an other straight objects Section 1 Equations of lines in What ou nee to know alrea: The ot prouct. The corresponence between equations an graphs.

More information

Chapter 2 Lagrangian Modeling

Chapter 2 Lagrangian Modeling Chapter 2 Lagrangian Moeling The basic laws of physics are use to moel every system whether it is electrical, mechanical, hyraulic, or any other energy omain. In mechanics, Newton s laws of motion provie

More information

SYMPLECTIC GEOMETRY: LECTURE 3

SYMPLECTIC GEOMETRY: LECTURE 3 SYMPLECTIC GEOMETRY: LECTURE 3 LIAT KESSLER 1. Local forms Vector fiels an the Lie erivative. A vector fiel on a manifol M is a smooth assignment of a vector tangent to M at each point. We think of M as

More information

ELEC3114 Control Systems 1

ELEC3114 Control Systems 1 ELEC34 Control Systems Linear Systems - Moelling - Some Issues Session 2, 2007 Introuction Linear systems may be represente in a number of ifferent ways. Figure shows the relationship between various representations.

More information

Schrödinger s equation.

Schrödinger s equation. Physics 342 Lecture 5 Schröinger s Equation Lecture 5 Physics 342 Quantum Mechanics I Wenesay, February 3r, 2010 Toay we iscuss Schröinger s equation an show that it supports the basic interpretation of

More information

Nöether s Theorem Under the Legendre Transform by Jonathan Herman

Nöether s Theorem Under the Legendre Transform by Jonathan Herman Nöether s Theorem Uner the Legenre Transform by Jonathan Herman A research paper presente to the University of Waterloo in fulfilment of the research paper requirement for the egree of Master of Mathematics

More information

Introduction to variational calculus: Lecture notes 1

Introduction to variational calculus: Lecture notes 1 October 10, 2006 Introuction to variational calculus: Lecture notes 1 Ewin Langmann Mathematical Physics, KTH Physics, AlbaNova, SE-106 91 Stockholm, Sween Abstract I give an informal summary of variational

More information

ANALYSIS OF A GENERAL FAMILY OF REGULARIZED NAVIER-STOKES AND MHD MODELS

ANALYSIS OF A GENERAL FAMILY OF REGULARIZED NAVIER-STOKES AND MHD MODELS ANALYSIS OF A GENERAL FAMILY OF REGULARIZED NAVIER-STOKES AND MHD MODELS MICHAEL HOLST, EVELYN LUNASIN, AND GANTUMUR TSOGTGEREL ABSTRACT. We consier a general family of regularize Navier-Stokes an Magnetohyroynamics

More information

Lower bounds on Locality Sensitive Hashing

Lower bounds on Locality Sensitive Hashing Lower bouns on Locality Sensitive Hashing Rajeev Motwani Assaf Naor Rina Panigrahy Abstract Given a metric space (X, X ), c 1, r > 0, an p, q [0, 1], a istribution over mappings H : X N is calle a (r,

More information

On the number of isolated eigenvalues of a pair of particles in a quantum wire

On the number of isolated eigenvalues of a pair of particles in a quantum wire On the number of isolate eigenvalues of a pair of particles in a quantum wire arxiv:1812.11804v1 [math-ph] 31 Dec 2018 Joachim Kerner 1 Department of Mathematics an Computer Science FernUniversität in

More information

Linear and quadratic approximation

Linear and quadratic approximation Linear an quaratic approximation November 11, 2013 Definition: Suppose f is a function that is ifferentiable on an interval I containing the point a. The linear approximation to f at a is the linear function

More information

Calculus in the AP Physics C Course The Derivative

Calculus in the AP Physics C Course The Derivative Limits an Derivatives Calculus in the AP Physics C Course The Derivative In physics, the ieas of the rate change of a quantity (along with the slope of a tangent line) an the area uner a curve are essential.

More information

ON THE GEOMETRIC APPROACH TO THE MOTION OF INERTIAL MECHANICAL SYSTEMS

ON THE GEOMETRIC APPROACH TO THE MOTION OF INERTIAL MECHANICAL SYSTEMS ON THE GEOMETRIC APPROACH TO THE MOTION OF INERTIAL MECHANICAL SYSTEMS ADRIAN CONSTANTIN AND BORIS KOLEV Abstract. Accoring to the principle of least action, the spatially perioic motions of one-imensional

More information

Lecture 2 Lagrangian formulation of classical mechanics Mechanics

Lecture 2 Lagrangian formulation of classical mechanics Mechanics Lecture Lagrangian formulation of classical mechanics 70.00 Mechanics Principle of stationary action MATH-GA To specify a motion uniquely in classical mechanics, it suffices to give, at some time t 0,

More information

Relation between the propagator matrix of geodesic deviation and the second-order derivatives of the characteristic function

Relation between the propagator matrix of geodesic deviation and the second-order derivatives of the characteristic function Journal of Electromagnetic Waves an Applications 203 Vol. 27 No. 3 589 60 http://x.oi.org/0.080/0920507.203.808595 Relation between the propagator matrix of geoesic eviation an the secon-orer erivatives

More information

Physics 5153 Classical Mechanics. The Virial Theorem and The Poisson Bracket-1

Physics 5153 Classical Mechanics. The Virial Theorem and The Poisson Bracket-1 Physics 5153 Classical Mechanics The Virial Theorem an The Poisson Bracket 1 Introuction In this lecture we will consier two applications of the Hamiltonian. The first, the Virial Theorem, applies to systems

More information

The Natural Logarithm

The Natural Logarithm The Natural Logarithm -28-208 In earlier courses, you may have seen logarithms efine in terms of raising bases to powers. For eample, log 2 8 = 3 because 2 3 = 8. In those terms, the natural logarithm

More information

arxiv: v2 [math.dg] 16 Dec 2014

arxiv: v2 [math.dg] 16 Dec 2014 A ONOTONICITY FORULA AND TYPE-II SINGULARITIES FOR THE EAN CURVATURE FLOW arxiv:1312.4775v2 [math.dg] 16 Dec 2014 YONGBING ZHANG Abstract. In this paper, we introuce a monotonicity formula for the mean

More information

GLOBAL SOLUTIONS FOR 2D COUPLED BURGERS-COMPLEX-GINZBURG-LANDAU EQUATIONS

GLOBAL SOLUTIONS FOR 2D COUPLED BURGERS-COMPLEX-GINZBURG-LANDAU EQUATIONS Electronic Journal of Differential Equations, Vol. 015 015), No. 99, pp. 1 14. ISSN: 107-6691. URL: http://eje.math.txstate.eu or http://eje.math.unt.eu ftp eje.math.txstate.eu GLOBAL SOLUTIONS FOR D COUPLED

More information

Linear First-Order Equations

Linear First-Order Equations 5 Linear First-Orer Equations Linear first-orer ifferential equations make up another important class of ifferential equations that commonly arise in applications an are relatively easy to solve (in theory)

More information

arxiv: v1 [math.dg] 1 Nov 2015

arxiv: v1 [math.dg] 1 Nov 2015 DARBOUX-WEINSTEIN THEOREM FOR LOCALLY CONFORMALLY SYMPLECTIC MANIFOLDS arxiv:1511.00227v1 [math.dg] 1 Nov 2015 ALEXANDRA OTIMAN AND MIRON STANCIU Abstract. A locally conformally symplectic (LCS) form is

More information

Calculus of Variations

Calculus of Variations Calculus of Variations Lagrangian formalism is the main tool of theoretical classical mechanics. Calculus of Variations is a part of Mathematics which Lagrangian formalism is base on. In this section,

More information

ON THE OPTIMALITY SYSTEM FOR A 1 D EULER FLOW PROBLEM

ON THE OPTIMALITY SYSTEM FOR A 1 D EULER FLOW PROBLEM ON THE OPTIMALITY SYSTEM FOR A D EULER FLOW PROBLEM Eugene M. Cliff Matthias Heinkenschloss y Ajit R. Shenoy z Interisciplinary Center for Applie Mathematics Virginia Tech Blacksburg, Virginia 46 Abstract

More information

A global Implicit Function Theorem without initial point and its applications to control of non-affine systems of high dimensions

A global Implicit Function Theorem without initial point and its applications to control of non-affine systems of high dimensions J. Math. Anal. Appl. 313 (2006) 251 261 www.elsevier.com/locate/jmaa A global Implicit Function Theorem without initial point an its applications to control of non-affine systems of high imensions Weinian

More information

Differentiability, Computing Derivatives, Trig Review

Differentiability, Computing Derivatives, Trig Review Unit #3 : Differentiability, Computing Derivatives, Trig Review Goals: Determine when a function is ifferentiable at a point Relate the erivative graph to the the graph of an original function Compute

More information

The group of isometries of the French rail ways metric

The group of isometries of the French rail ways metric Stu. Univ. Babeş-Bolyai Math. 58(2013), No. 4, 445 450 The group of isometries of the French rail ways metric Vasile Bulgărean To the memory of Professor Mircea-Eugen Craioveanu (1942-2012) Abstract. In

More information

A nonlinear inverse problem of the Korteweg-de Vries equation

A nonlinear inverse problem of the Korteweg-de Vries equation Bull. Math. Sci. https://oi.org/0.007/s3373-08-025- A nonlinear inverse problem of the Korteweg-e Vries equation Shengqi Lu Miaochao Chen 2 Qilin Liu 3 Receive: 0 March 207 / Revise: 30 April 208 / Accepte:

More information

LATTICE-BASED D-OPTIMUM DESIGN FOR FOURIER REGRESSION

LATTICE-BASED D-OPTIMUM DESIGN FOR FOURIER REGRESSION The Annals of Statistics 1997, Vol. 25, No. 6, 2313 2327 LATTICE-BASED D-OPTIMUM DESIGN FOR FOURIER REGRESSION By Eva Riccomagno, 1 Rainer Schwabe 2 an Henry P. Wynn 1 University of Warwick, Technische

More information

Differentiability, Computing Derivatives, Trig Review. Goals:

Differentiability, Computing Derivatives, Trig Review. Goals: Secants vs. Derivatives - Unit #3 : Goals: Differentiability, Computing Derivatives, Trig Review Determine when a function is ifferentiable at a point Relate the erivative graph to the the graph of an

More information

Differentiation ( , 9.5)

Differentiation ( , 9.5) Chapter 2 Differentiation (8.1 8.3, 9.5) 2.1 Rate of Change (8.2.1 5) Recall that the equation of a straight line can be written as y = mx + c, where m is the slope or graient of the line, an c is the

More information

Abstract A nonlinear partial differential equation of the following form is considered:

Abstract A nonlinear partial differential equation of the following form is considered: M P E J Mathematical Physics Electronic Journal ISSN 86-6655 Volume 2, 26 Paper 5 Receive: May 3, 25, Revise: Sep, 26, Accepte: Oct 6, 26 Eitor: C.E. Wayne A Nonlinear Heat Equation with Temperature-Depenent

More information

Second order differentiation formula on RCD(K, N) spaces

Second order differentiation formula on RCD(K, N) spaces Secon orer ifferentiation formula on RCD(K, N) spaces Nicola Gigli Luca Tamanini February 8, 018 Abstract We prove the secon orer ifferentiation formula along geoesics in finite-imensional RCD(K, N) spaces.

More information

Linear Algebra- Review And Beyond. Lecture 3

Linear Algebra- Review And Beyond. Lecture 3 Linear Algebra- Review An Beyon Lecture 3 This lecture gives a wie range of materials relate to matrix. Matrix is the core of linear algebra, an it s useful in many other fiels. 1 Matrix Matrix is the

More information

MARKO NEDELJKOV, DANIJELA RAJTER-ĆIRIĆ

MARKO NEDELJKOV, DANIJELA RAJTER-ĆIRIĆ GENERALIZED UNIFORMLY CONTINUOUS SEMIGROUPS AND SEMILINEAR HYPERBOLIC SYSTEMS WITH REGULARIZED DERIVATIVES MARKO NEDELJKOV, DANIJELA RAJTER-ĆIRIĆ Abstract. We aopt the theory of uniformly continuous operator

More information

Tractability results for weighted Banach spaces of smooth functions

Tractability results for weighted Banach spaces of smooth functions Tractability results for weighte Banach spaces of smooth functions Markus Weimar Mathematisches Institut, Universität Jena Ernst-Abbe-Platz 2, 07740 Jena, Germany email: markus.weimar@uni-jena.e March

More information

Notes on Lie Groups, Lie algebras, and the Exponentiation Map Mitchell Faulk

Notes on Lie Groups, Lie algebras, and the Exponentiation Map Mitchell Faulk Notes on Lie Groups, Lie algebras, an the Exponentiation Map Mitchell Faulk 1. Preliminaries. In these notes, we concern ourselves with special objects calle matrix Lie groups an their corresponing Lie

More information

Final Exam Study Guide and Practice Problems Solutions

Final Exam Study Guide and Practice Problems Solutions Final Exam Stuy Guie an Practice Problems Solutions Note: These problems are just some of the types of problems that might appear on the exam. However, to fully prepare for the exam, in aition to making

More information

Stable and compact finite difference schemes

Stable and compact finite difference schemes Center for Turbulence Research Annual Research Briefs 2006 2 Stable an compact finite ifference schemes By K. Mattsson, M. Svär AND M. Shoeybi. Motivation an objectives Compact secon erivatives have long

More information

A Novel Decoupled Iterative Method for Deep-Submicron MOSFET RF Circuit Simulation

A Novel Decoupled Iterative Method for Deep-Submicron MOSFET RF Circuit Simulation A Novel ecouple Iterative Metho for eep-submicron MOSFET RF Circuit Simulation CHUAN-SHENG WANG an YIMING LI epartment of Mathematics, National Tsing Hua University, National Nano evice Laboratories, an

More information

d dx [xn ] = nx n 1. (1) dy dx = 4x4 1 = 4x 3. Theorem 1.3 (Derivative of a constant function). If f(x) = k and k is a constant, then f (x) = 0.

d dx [xn ] = nx n 1. (1) dy dx = 4x4 1 = 4x 3. Theorem 1.3 (Derivative of a constant function). If f(x) = k and k is a constant, then f (x) = 0. Calculus refresher Disclaimer: I claim no original content on this ocument, which is mostly a summary-rewrite of what any stanar college calculus book offers. (Here I ve use Calculus by Dennis Zill.) I

More information

SINGULAR PERTURBATION AND STATIONARY SOLUTIONS OF PARABOLIC EQUATIONS IN GAUSS-SOBOLEV SPACES

SINGULAR PERTURBATION AND STATIONARY SOLUTIONS OF PARABOLIC EQUATIONS IN GAUSS-SOBOLEV SPACES Communications on Stochastic Analysis Vol. 2, No. 2 (28) 289-36 Serials Publications www.serialspublications.com SINGULAR PERTURBATION AND STATIONARY SOLUTIONS OF PARABOLIC EQUATIONS IN GAUSS-SOBOLEV SPACES

More information

LECTURE NOTES ON DVORETZKY S THEOREM

LECTURE NOTES ON DVORETZKY S THEOREM LECTURE NOTES ON DVORETZKY S THEOREM STEVEN HEILMAN Abstract. We present the first half of the paper [S]. In particular, the results below, unless otherwise state, shoul be attribute to G. Schechtman.

More information

. ISSN (print), (online) International Journal of Nonlinear Science Vol.6(2008) No.3,pp

. ISSN (print), (online) International Journal of Nonlinear Science Vol.6(2008) No.3,pp . ISSN 1749-3889 (print), 1749-3897 (online) International Journal of Nonlinear Science Vol.6(8) No.3,pp.195-1 A Bouneness Criterion for Fourth Orer Nonlinear Orinary Differential Equations with Delay

More information

LOCAL AND GLOBAL MINIMALITY RESULTS FOR A NONLOCAL ISOPERIMETRIC PROBLEM ON R N

LOCAL AND GLOBAL MINIMALITY RESULTS FOR A NONLOCAL ISOPERIMETRIC PROBLEM ON R N LOCAL AND GLOBAL MINIMALITY RSULTS FOR A NONLOCAL ISOPRIMTRIC PROBLM ON R N M. BONACINI AND R. CRISTOFRI Abstract. We consier a nonlocal isoperimetric problem efine in the whole space R N, whose nonlocal

More information

Math Notes on differentials, the Chain Rule, gradients, directional derivative, and normal vectors

Math Notes on differentials, the Chain Rule, gradients, directional derivative, and normal vectors Math 18.02 Notes on ifferentials, the Chain Rule, graients, irectional erivative, an normal vectors Tangent plane an linear approximation We efine the partial erivatives of f( xy, ) as follows: f f( x+

More information

Switching Time Optimization in Discretized Hybrid Dynamical Systems

Switching Time Optimization in Discretized Hybrid Dynamical Systems Switching Time Optimization in Discretize Hybri Dynamical Systems Kathrin Flaßkamp, To Murphey, an Sina Ober-Blöbaum Abstract Switching time optimization (STO) arises in systems that have a finite set

More information

WUCHEN LI AND STANLEY OSHER

WUCHEN LI AND STANLEY OSHER CONSTRAINED DYNAMICAL OPTIMAL TRANSPORT AND ITS LAGRANGIAN FORMULATION WUCHEN LI AND STANLEY OSHER Abstract. We propose ynamical optimal transport (OT) problems constraine in a parameterize probability

More information

Introduction to the Vlasov-Poisson system

Introduction to the Vlasov-Poisson system Introuction to the Vlasov-Poisson system Simone Calogero 1 The Vlasov equation Consier a particle with mass m > 0. Let x(t) R 3 enote the position of the particle at time t R an v(t) = ẋ(t) = x(t)/t its

More information

Math 342 Partial Differential Equations «Viktor Grigoryan

Math 342 Partial Differential Equations «Viktor Grigoryan Math 342 Partial Differential Equations «Viktor Grigoryan 6 Wave equation: solution In this lecture we will solve the wave equation on the entire real line x R. This correspons to a string of infinite

More information

11.7. Implicit Differentiation. Introduction. Prerequisites. Learning Outcomes

11.7. Implicit Differentiation. Introduction. Prerequisites. Learning Outcomes Implicit Differentiation 11.7 Introuction This Section introuces implicit ifferentiation which is use to ifferentiate functions expresse in implicit form (where the variables are foun together). Examples

More information

Mathematical Review Problems

Mathematical Review Problems Fall 6 Louis Scuiero Mathematical Review Problems I. Polynomial Equations an Graphs (Barrante--Chap. ). First egree equation an graph y f() x mx b where m is the slope of the line an b is the line's intercept

More information

Many problems in physics, engineering, and chemistry fall in a general class of equations of the form. d dx. d dx

Many problems in physics, engineering, and chemistry fall in a general class of equations of the form. d dx. d dx Math 53 Notes on turm-liouville equations Many problems in physics, engineering, an chemistry fall in a general class of equations of the form w(x)p(x) u ] + (q(x) λ) u = w(x) on an interval a, b], plus

More information

Integration Review. May 11, 2013

Integration Review. May 11, 2013 Integration Review May 11, 2013 Goals: Review the funamental theorem of calculus. Review u-substitution. Review integration by parts. Do lots of integration eamples. 1 Funamental Theorem of Calculus In

More information

INVERSE PROBLEM OF A HYPERBOLIC EQUATION WITH AN INTEGRAL OVERDETERMINATION CONDITION

INVERSE PROBLEM OF A HYPERBOLIC EQUATION WITH AN INTEGRAL OVERDETERMINATION CONDITION Electronic Journal of Differential Equations, Vol. 216 (216), No. 138, pp. 1 7. ISSN: 172-6691. URL: http://eje.math.txstate.eu or http://eje.math.unt.eu INVERSE PROBLEM OF A HYPERBOLIC EQUATION WITH AN

More information

Calculus of Variations

Calculus of Variations 16.323 Lecture 5 Calculus of Variations Calculus of Variations Most books cover this material well, but Kirk Chapter 4 oes a particularly nice job. x(t) x* x*+ αδx (1) x*- αδx (1) αδx (1) αδx (1) t f t

More information

Optimal A Priori Discretization Error Bounds for Geodesic Finite Elements

Optimal A Priori Discretization Error Bounds for Geodesic Finite Elements Optimal A Priori iscretization Error Bouns for Geoesic Finite Elements Philipp Grohs, Hanne Harering an Oliver Saner Bericht Nr. 365 Mai 13 Key wors: geoesic finite elements, iscretization error, a priori

More information

Distribution Theory for Discontinuous Test Functions and Differential Operators with Generalized Coefficients

Distribution Theory for Discontinuous Test Functions and Differential Operators with Generalized Coefficients JOURNAL OF MATHEMATICAL ANALYSIS AND APPLICATIONS 1, 9733 1996 ARTICLE NO 56 Distribution Theory for Discontinuous Test Functions an Differential Operators with Generalize Coefficients P Kurasov* Department

More information

Derivatives and the Product Rule

Derivatives and the Product Rule Derivatives an the Prouct Rule James K. Peterson Department of Biological Sciences an Department of Mathematical Sciences Clemson University January 28, 2014 Outline Differentiability Simple Derivatives

More information

Calculus I Practice Test Problems for Chapter 3 Page 1 of 9

Calculus I Practice Test Problems for Chapter 3 Page 1 of 9 Calculus I Practice Test Problems for Chapter 3 Page of 9 This is a set of practice test problems for Chapter 3. This is in no wa an inclusive set of problems there can be other tpes of problems on the

More information

Dissipative numerical methods for the Hunter-Saxton equation

Dissipative numerical methods for the Hunter-Saxton equation Dissipative numerical methos for the Hunter-Saton equation Yan Xu an Chi-Wang Shu Abstract In this paper, we present further evelopment of the local iscontinuous Galerkin (LDG) metho esigne in [] an a

More information

ALGEBRAIC AND ANALYTIC PROPERTIES OF ARITHMETIC FUNCTIONS

ALGEBRAIC AND ANALYTIC PROPERTIES OF ARITHMETIC FUNCTIONS ALGEBRAIC AND ANALYTIC PROPERTIES OF ARITHMETIC FUNCTIONS MARK SCHACHNER Abstract. When consiere as an algebraic space, the set of arithmetic functions equippe with the operations of pointwise aition an

More information

Convergence of Random Walks

Convergence of Random Walks Chapter 16 Convergence of Ranom Walks This lecture examines the convergence of ranom walks to the Wiener process. This is very important both physically an statistically, an illustrates the utility of

More information

Witten s Proof of Morse Inequalities

Witten s Proof of Morse Inequalities Witten s Proof of Morse Inequalities by Igor Prokhorenkov Let M be a smooth, compact, oriente manifol with imension n. A Morse function is a smooth function f : M R such that all of its critical points

More information

Lecture 6: Calculus. In Song Kim. September 7, 2011

Lecture 6: Calculus. In Song Kim. September 7, 2011 Lecture 6: Calculus In Song Kim September 7, 20 Introuction to Differential Calculus In our previous lecture we came up with several ways to analyze functions. We saw previously that the slope of a linear

More information

TRAJECTORY TRACKING FOR FULLY ACTUATED MECHANICAL SYSTEMS

TRAJECTORY TRACKING FOR FULLY ACTUATED MECHANICAL SYSTEMS TRAJECTORY TRACKING FOR FULLY ACTUATED MECHANICAL SYSTEMS Francesco Bullo Richar M. Murray Control an Dynamical Systems California Institute of Technology Pasaena, CA 91125 Fax : + 1-818-796-8914 email

More information

Harmonic Modelling of Thyristor Bridges using a Simplified Time Domain Method

Harmonic Modelling of Thyristor Bridges using a Simplified Time Domain Method 1 Harmonic Moelling of Thyristor Briges using a Simplifie Time Domain Metho P. W. Lehn, Senior Member IEEE, an G. Ebner Abstract The paper presents time omain methos for harmonic analysis of a 6-pulse

More information

12.11 Laplace s Equation in Cylindrical and

12.11 Laplace s Equation in Cylindrical and SEC. 2. Laplace s Equation in Cylinrical an Spherical Coorinates. Potential 593 2. Laplace s Equation in Cylinrical an Spherical Coorinates. Potential One of the most important PDEs in physics an engineering

More information

Approximate reduction of dynamic systems

Approximate reduction of dynamic systems Systems & Control Letters 57 2008 538 545 www.elsevier.com/locate/sysconle Approximate reuction of ynamic systems Paulo Tabuaa a,, Aaron D. Ames b, Agung Julius c, George J. Pappas c a Department of Electrical

More information

Optimal Control of Spatially Distributed Systems

Optimal Control of Spatially Distributed Systems Optimal Control of Spatially Distribute Systems Naer Motee an Ali Jababaie Abstract In this paper, we stuy the structural properties of optimal control of spatially istribute systems. Such systems consist

More information

The Principle of Least Action

The Principle of Least Action Chapter 7. The Principle of Least Action 7.1 Force Methos vs. Energy Methos We have so far stuie two istinct ways of analyzing physics problems: force methos, basically consisting of the application of

More information

Federer s characterization of sets of finite perimeter in metric spaces

Federer s characterization of sets of finite perimeter in metric spaces Feerer s characterization of sets of finite perimeter in metric spaces Panu Lahti April 28, 208 Abstract Feerer s characterization of sets of finite perimeter states (in Eucliean spaces) that a set is

More information

arxiv: v1 [math-ph] 5 May 2014

arxiv: v1 [math-ph] 5 May 2014 DIFFERENTIAL-ALGEBRAIC SOLUTIONS OF THE HEAT EQUATION VICTOR M. BUCHSTABER, ELENA YU. NETAY arxiv:1405.0926v1 [math-ph] 5 May 2014 Abstract. In this work we introuce the notion of ifferential-algebraic

More information

The Non-abelian Hodge Correspondence for Non-Compact Curves

The Non-abelian Hodge Correspondence for Non-Compact Curves 1 Section 1 Setup The Non-abelian Hoge Corresponence for Non-Compact Curves Chris Elliott May 8, 2011 1 Setup In this talk I will escribe the non-abelian Hoge theory of a non-compact curve. This was worke

More information

WELL-POSEDNESS OF A POROUS MEDIUM FLOW WITH FRACTIONAL PRESSURE IN SOBOLEV SPACES

WELL-POSEDNESS OF A POROUS MEDIUM FLOW WITH FRACTIONAL PRESSURE IN SOBOLEV SPACES Electronic Journal of Differential Equations, Vol. 017 (017), No. 38, pp. 1 7. ISSN: 107-6691. URL: http://eje.math.txstate.eu or http://eje.math.unt.eu WELL-POSEDNESS OF A POROUS MEDIUM FLOW WITH FRACTIONAL

More information

Mark J. Machina CARDINAL PROPERTIES OF "LOCAL UTILITY FUNCTIONS"

Mark J. Machina CARDINAL PROPERTIES OF LOCAL UTILITY FUNCTIONS Mark J. Machina CARDINAL PROPERTIES OF "LOCAL UTILITY FUNCTIONS" This paper outlines the carinal properties of "local utility functions" of the type use by Allen [1985], Chew [1983], Chew an MacCrimmon

More information

Energy behaviour of the Boris method for charged-particle dynamics

Energy behaviour of the Boris method for charged-particle dynamics Version of 25 April 218 Energy behaviour of the Boris metho for charge-particle ynamics Ernst Hairer 1, Christian Lubich 2 Abstract The Boris algorithm is a wiely use numerical integrator for the motion

More information

Math 1271 Solutions for Fall 2005 Final Exam

Math 1271 Solutions for Fall 2005 Final Exam Math 7 Solutions for Fall 5 Final Eam ) Since the equation + y = e y cannot be rearrange algebraically in orer to write y as an eplicit function of, we must instea ifferentiate this relation implicitly

More information

Qubit channels that achieve capacity with two states

Qubit channels that achieve capacity with two states Qubit channels that achieve capacity with two states Dominic W. Berry Department of Physics, The University of Queenslan, Brisbane, Queenslan 4072, Australia Receive 22 December 2004; publishe 22 March

More information

Exam 2 Answers Math , Fall log x dx = x log x x + C. log u du = 1 3

Exam 2 Answers Math , Fall log x dx = x log x x + C. log u du = 1 3 Exam Answers Math -, Fall 7. Show, using any metho you like, that log x = x log x x + C. Answer: (x log x x+c) = x x + log x + = log x. Thus log x = x log x x+c.. Compute these. Remember to put boxes aroun

More information

Exponential asymptotic property of a parallel repairable system with warm standby under common-cause failure

Exponential asymptotic property of a parallel repairable system with warm standby under common-cause failure J. Math. Anal. Appl. 341 (28) 457 466 www.elsevier.com/locate/jmaa Exponential asymptotic property of a parallel repairable system with warm stanby uner common-cause failure Zifei Shen, Xiaoxiao Hu, Weifeng

More information