Using Bernoulli Equation to Solve Burger's Equation

Size: px
Start display at page:

Download "Using Bernoulli Equation to Solve Burger's Equation"

Transcription

1 Vol.() Using Bernoulli Equation to Solve Burger's Equation Saad N. AL-Azawi* Muna Saleh * Received, December, Accepted, June, Abstract: In this paper we find the exact solution of Burger's equation after reducing it to Bernoulli equation. We compare this solution with that given by Kaya where he used Adomian decomposition method, the solution given by chakrone where he used the Variation iteration method (VIM)and the solution given by Eq()in the paper of M. Javidi. We notice that our solution is better than their solutions. Key words: Burger's equation, kdv equation, PDF.. Introduction: We consider the following Burger's equation is positive parameter This equation arises in various areas of science. Equation (.) has been used in the study of the propagation through liquid-filled elastic tube[].and description for shallow water waves on a viscous fluid [].Equation(.)is used as a model for traffic flow [].Many Researchers had proposed various kinds of exact and numerical solution [,,6,7,8,9,] where they used Adomian decomposition method, variation iteration method, Galerkin method.. Derivation of Burger's equation.[9] We recall the differential form of the nonlinear conservation equation and allow a jump discontinuity for p and q. In many physical problems of interest it would be a better approximation to assume that q is a function of the density gradient as well as p.a simple model is to take is a positive constant.substituting (.) into (.), we obtain the nonlinear diffusion equation, We multiply (.) by Hence: And therefore: to obtain To investigate the nature of the discontinuous solution or shock waves, we assume a function relation If is a quadratic function in,then is linear in p, and. Consequently (.) * Department of Mathematics. College of science for women. Baghdad University

2 Vol.() As a simple model of turbulence, is replaced by the fluid velocity field to obtain the well-known Burgers equation as i.e. is the kinematic viscosity.thus,the Burgers equation is a balance between time evaluation, nonlinearity and diffusion.. Solution of Burger's equation. To solve Burger's equation (.), we can assume the solution c is an arbitrary constant. Hence, from (.) we get Now, let [In order to eliminate c from equation (.)] substituting (.6) into (.) i.e. - is called the travelling wave solution-substituting (.) into (.) Let to get Rewrite (.) as a system of first order O.D.E s Let Then (.7) represent the velocity and a acceleration respectively. Then Notice that equation (.9) represents Bernoulli equation. To solve it Suppose Substituting (.) into (.9) This system has an infinite number of equilibrium points which is axis To solve (.) divide the two equations to get We get

3 This equation is first-order linear differential equation, its integrating factor is And its solution is gives by Vol.() BC: BC: Clearly u (, ) = (stationary case) BC so, is an arbitrary constant BC From (.), we get the solution of Bernoulli equation (.9) By using (.6) and (.) Now, from (.6) so the traveling wave solution (.) Therefore, Remember that from (.8) k is given in (.8) and an arbitrary constant where are arbitrary constants. And. The solution of Burger's equation with Dirichlet conditions. From (.) the solution of Burger's equation is Dirichlet conditions are is And from (.) From which we get From(.) and (.)we determine After determining these constants we

4 find the solution of Burger's equation with Dirichlet conditions. As a special case let then from (.8) we get Vol.() solution, while our solution is exact solution. The solution obtained by Javidi And from (.) we get Or Case : Case: when, A=, B= ) and C=,k=., c= Clearly our solution is easier than his solution. in the solution function α=-.7, =. The graphs of (.),(.6) are in figures ()and() respectively. The two shapes have the same qualitative behavior but quantitavely different. where t=[:.:.],x=[-::] This figure classifies the wave at the beginning of the earth quake..comparison. The solution of this equation obtained by Kaya where is not easier than our solution. The solution obtained by Omar is approximated

5 Case : - Case: - Fig.-- Fig.-- References:. R.S.Jonson, 97.A Non Linear Equation Incorporating Damping and Disper sion.j.phys.mech.()9-6.. R.S.Jonson, 97.Shallow Water Wave in Viscous Fluid-the Undular Bore.phys- Fluids () Vol.(). Md Abdur Rab,.Some Travelling Wave Solutions of KdV- Burgers Equation.Int. Journal of Math. Analysis, Vol. 6(): - 6. Dogan Kaya,.An application of the decomposition method for the KdVB Equation.Applied Mathematics and Computation () Omar Chakrone, Okacha Diyer, Driss Sbibih.Improved numerical solution of Burger's equation.bol.soc.paran.mat. (s)v.8 ():9-6. J.Biazar and H.H.Ghazvini, 9.Exact and numerical for non - linear Burger's Equation by VIM. Mathematical and Computer Modelling, J.H.He, 7.Variational iteration method - Some recent results and new inter-pretations. Mathematical Computer. 8. X.H.Zhang, J.Ouyang, L.Zhang, 9.Element - free characteristic Galerkin method for Buger's equation. Engineering Analysis with Boundary Elements, Jawad Kadhim, 7.Non-Classical Variation Formulation Approach for solving one-dimensional Non linear Partial Differential Burger's Problem.M.S.C thesis, Baghdad University. M. Javidi, 6.A numerical solution of Burgers equation based on modied extended BDF scheme. International Mathematical Forum, ( )6-7 استخدام معادلة برنو لي لحل معادلة بيركر سعد ناجي العزاوي* *قسم الرياضيات كلية العلوم للبنات جامعة بغداد. منى صالح* الخالصة: حصلنا من بحثنا هذا على الحل المضبوط )Exact( لمعادلة بيركر بعد تحويلها إلى معادلة برنو لي وتمت مقارنة هذا الحل مع حل " Kaya "الذي استخدم طريقة تجزئة ادومين وحل "Chakrone" الذي أستخدم طريقة التغاير المتكرر وحل "Javidi" المعطى بالعالقة ) (وتبين ان حلنا هذا افضل من حلولهم للبساطه الصيغة

The Modified Quadrature Method for solving Volterra Linear Integral Equations

The Modified Quadrature Method for solving Volterra Linear Integral Equations The Modified Quadrature Method for solving Volterra Linear Integral Equations Mahmood A. Shamran* Sami Abdulla Abid** Received 15, January, 2014 Accepted 30, March, 2014 Abstract: In this paper the modified

More information

On Solving Singular Multi Point Boundary Value Problems with Nonlocal Condition حول حل مسائل القيم الحدودية متعددة النقاط الشاذة مع شروط

On Solving Singular Multi Point Boundary Value Problems with Nonlocal Condition حول حل مسائل القيم الحدودية متعددة النقاط الشاذة مع شروط ISSN: 0067-2904 GIF: 0.851 On Solving Singular Multi Point Boundary Value Problems with Nonlocal Condition Heba. A. Abd Al-Razak* Department of Mathematics, College of Science for Women, Baghdad University,

More information

On Right α-centralizers and Commutativity of Prime Rings

On Right α-centralizers and Commutativity of Prime Rings On Right α-centralizers and Commutativity of Prime Rings Amira A. Abduljaleel*, Abdulrahman H. Majeed Department of Mathematics, College of Science, Baghdad University, Baghdad, Iraq Abstract: Let R be

More information

- Primary Submodules

- Primary Submodules - Primary Submodules Nuhad Salim Al-Mothafar*, Ali Talal Husain Department of Mathematics, College of Science, University of Baghdad, Baghdad, Iraq Abstract Let is a commutative ring with identity and

More information

A New Operational Matrix of Derivative for Orthonormal Bernstein Polynomial's

A New Operational Matrix of Derivative for Orthonormal Bernstein Polynomial's A New Operational Matrix of Derivative for Orthonormal Bernstein Polynomial's MayadaN.Mohammed Ali* Received 16, May, 2013 Accepted 26, September, 2013 Abstract: In this paper, an orthonormal family has

More information

Oscillations of First Order Neutral Differential Equations with Positive and Negative Coefficients

Oscillations of First Order Neutral Differential Equations with Positive and Negative Coefficients Oscillations of First Order Neutral Differential Equations with Positive and Negative Coefficients Hussain Ali Mohamad* MuntahaYousif Abdullah** Received 21, May, 2013 Accepted 2, October, 2013 Abstract:

More information

x y = 2 x + 2y = 14 x = 2, y = 0 x = 3, y = 1 x = 4, y = 2 x = 5, y = 3 x = 6, y = 4 x = 7, y = 5 x = 0, y = 7 x = 2, y = 6 x = 4, y = 5

x y = 2 x + 2y = 14 x = 2, y = 0 x = 3, y = 1 x = 4, y = 2 x = 5, y = 3 x = 6, y = 4 x = 7, y = 5 x = 0, y = 7 x = 2, y = 6 x = 4, y = 5 List six positive integer solutions for each of these equations and comment on your results. Two have been done for you. x y = x + y = 4 x =, y = 0 x = 3, y = x = 4, y = x = 5, y = 3 x = 6, y = 4 x = 7,

More information

Applications of Variational Iteration Method for Solving A Class of Volterra Integral Equations

Applications of Variational Iteration Method for Solving A Class of Volterra Integral Equations Applications of Variational Iteration Method for Solving A Class of Volterra Integral Equations Mohammed S. Mechee Adil M. Al Ramahi Raad M. Kadum Department of Math., Faculty of Computer Science and Math.,

More information

Volterra Runge- Kutta Methods for Solving Nonlinear Volterra Integral Equations

Volterra Runge- Kutta Methods for Solving Nonlinear Volterra Integral Equations Volterra Runge- Kutta Methods for Solving Nonlinear Volterra Integral Equations Muna M. Mustafa* Received 17, March, 2009 Acceptance 22, June, 2009 Abstract: In this paper Volterra Runge-Kutta methods

More information

Exponential Function of a bounded Linear Operator on a Hilbert Space.

Exponential Function of a bounded Linear Operator on a Hilbert Space. Exponential Function of a bounded Linear Operator on a Hilbert Space. Radhi I. Mohammed * Fatin A. Ahmed ** Received 28, May, 2013 Accepted 18, September, 2013 Abstract: In this paper, we introduce an

More information

The Modified Variational Iteration Method for Solving Linear and Nonlinear Ordinary Differential Equations

The Modified Variational Iteration Method for Solving Linear and Nonlinear Ordinary Differential Equations Australian Journal of Basic and Applied Sciences, 5(10): 406-416, 2011 ISSN 1991-8178 The Modified Variational Iteration Method for Solving Linear and Nonlinear Ordinary Differential Equations 1 M.A. Fariborzi

More information

B-splines Collocation Algorithms for Solving Numerically the MRLW Equation

B-splines Collocation Algorithms for Solving Numerically the MRLW Equation ISSN 1749-889 (print), 1749-897 (online) International Journal of Nonlinear Science Vol.8(2009) No.2,pp.11-140 B-splines Collocation Algorithms for Solving Numerically the MRLW Equation Saleh M. Hassan,

More information

Notes: Outline. Shock formation. Notes: Notes: Shocks in traffic flow

Notes: Outline. Shock formation. Notes: Notes: Shocks in traffic flow Outline Scalar nonlinear conservation laws Traffic flow Shocks and rarefaction waves Burgers equation Rankine-Hugoniot conditions Importance of conservation form Weak solutions Reading: Chapter, 2 R.J.

More information

Gas Dynamics: Basic Equations, Waves and Shocks

Gas Dynamics: Basic Equations, Waves and Shocks Astrophysical Dynamics, VT 010 Gas Dynamics: Basic Equations, Waves and Shocks Susanne Höfner Susanne.Hoefner@fysast.uu.se Astrophysical Dynamics, VT 010 Gas Dynamics: Basic Equations, Waves and Shocks

More information

Bit-Plane Slicing Autoregressive Modeling for Medical Image Compression نموذج تشريح البتات واالنحدار الذاتي لضغط الصور الطبية

Bit-Plane Slicing Autoregressive Modeling for Medical Image Compression نموذج تشريح البتات واالنحدار الذاتي لضغط الصور الطبية Bit-Plane Slicing Autoregressive Modeling for Medical Image Compression Saadoon Ghadah Al-Khafaji, Hussein Noori Department of Computer Science, College of Science, Baghdad University, Baghdad, Iraq Abstract

More information

The variational homotopy perturbation method for solving the K(2,2)equations

The variational homotopy perturbation method for solving the K(2,2)equations International Journal of Applied Mathematical Research, 2 2) 213) 338-344 c Science Publishing Corporation wwwsciencepubcocom/indexphp/ijamr The variational homotopy perturbation method for solving the

More information

Linear Variable coefficient equations (Sect. 2.1) Review: Linear constant coefficient equations

Linear Variable coefficient equations (Sect. 2.1) Review: Linear constant coefficient equations Linear Variable coefficient equations (Sect. 2.1) Review: Linear constant coefficient equations. The Initial Value Problem. Linear variable coefficients equations. The Bernoulli equation: A nonlinear equation.

More information

Introduction to Partial Differential Equations

Introduction to Partial Differential Equations Introduction to Partial Differential Equations Philippe B. Laval KSU Current Semester Philippe B. Laval (KSU) 1D Heat Equation: Derivation Current Semester 1 / 19 Introduction The derivation of the heat

More information

13 PDEs on spatially bounded domains: initial boundary value problems (IBVPs)

13 PDEs on spatially bounded domains: initial boundary value problems (IBVPs) 13 PDEs on spatially bounded domains: initial boundary value problems (IBVPs) A prototypical problem we will discuss in detail is the 1D diffusion equation u t = Du xx < x < l, t > finite-length rod u(x,

More information

Alternative numerical method in continuum mechanics COMPUTATIONAL MULTISCALE. University of Liège Aerospace & Mechanical Engineering

Alternative numerical method in continuum mechanics COMPUTATIONAL MULTISCALE. University of Liège Aerospace & Mechanical Engineering University of Liège Aerospace & Mechanical Engineering Alternative numerical method in continuum mechanics COMPUTATIONAL MULTISCALE Van Dung NGUYEN Innocent NIYONZIMA Aerospace & Mechanical engineering

More information

Travelling waves. Chapter 8. 1 Introduction

Travelling waves. Chapter 8. 1 Introduction Chapter 8 Travelling waves 1 Introduction One of the cornerstones in the study of both linear and nonlinear PDEs is the wave propagation. A wave is a recognizable signal which is transferred from one part

More information

He's variational iteration method to approximate time fractional wave non linear like equation with variable coefficient

He's variational iteration method to approximate time fractional wave non linear like equation with variable coefficient He's variational iteration method to approximate time fractional wave non linear like equation with variable coefficient Abeer Majeed Jasim Department of Mathematics,College of science, university of Basrah,

More information

HOMOTOPY ANALYSIS METHOD FOR SOLVING KDV EQUATIONS

HOMOTOPY ANALYSIS METHOD FOR SOLVING KDV EQUATIONS Surveys in Mathematics and its Applications ISSN 1842-6298 (electronic), 1843-7265 (print) Volume 5 (21), 89 98 HOMOTOPY ANALYSIS METHOD FOR SOLVING KDV EQUATIONS Hossein Jafari and M. A. Firoozjaee Abstract.

More information

Linear Variable coefficient equations (Sect. 1.2) Review: Linear constant coefficient equations

Linear Variable coefficient equations (Sect. 1.2) Review: Linear constant coefficient equations Linear Variable coefficient equations (Sect. 1.2) Review: Linear constant coefficient equations. The Initial Value Problem. Linear variable coefficients equations. The Bernoulli equation: A nonlinear equation.

More information

A. Incorrect! Replacing is not a method for solving systems of equations.

A. Incorrect! Replacing is not a method for solving systems of equations. ACT Math and Science - Problem Drill 20: Systems of Equations No. 1 of 10 1. What methods were presented to solve systems of equations? (A) Graphing, replacing, and substitution. (B) Solving, replacing,

More information

The Solar Attraction Effect on Orbital Elements of the Moon

The Solar Attraction Effect on Orbital Elements of the Moon The Solar Attraction Effect on Orbital Elements of the Moon Abdulrahman H. Saleh*, Taif A. Damin Department of Astronomy and Space, College of Science, University of Baghdad, Baghdad, Iraq Abstract In

More information

Monte Carlo Simulation of the Effective Solid Angle and the HPGe Response to Different Mono-Energetic Protons from Extended Source.

Monte Carlo Simulation of the Effective Solid Angle and the HPGe Response to Different Mono-Energetic Protons from Extended Source. Monte Carlo Simulation of the Effective Solid Angle and the HPGe Response to Different Mono-Energetic Protons from Extended Source. Alaa B. Kadhim Department of Astronomy and Space, College of Science,

More information

The Approximation Solution of Some Calculus of Variation Problems Based Euler-Lagrange Equations

The Approximation Solution of Some Calculus of Variation Problems Based Euler-Lagrange Equations Variation Problems Based Euler-Lagrange Equations Zina Khalil Alabacy Control and System Engineering Department, University of Technology/ Baghdad. Email: zina_abacy@yahoo.com. Received on: 22/10/2014

More information

Solving Quadratic Equations

Solving Quadratic Equations Solving Quadratic Equations MATH 101 College Algebra J. Robert Buchanan Department of Mathematics Summer 2012 Objectives In this lesson we will learn to: solve quadratic equations by factoring, solve quadratic

More information

Analytical Study of near Mobility Edge Density of States of Hydrogenated Amorphous Silicon

Analytical Study of near Mobility Edge Density of States of Hydrogenated Amorphous Silicon Analytical Study of near Mobility Edge Density of States of Hydrogenated Amorphous Silicon Abdullah Ibrahim Abbo* Received 7, April, 2013 Accepted 12, November, 2013 Abstract: Experimental results for

More information

Quasi Duo Rings whose Every Simple Singular Modules is YJ-Injective حلقات كوازي ديو والتي كل مقاس بسيط منفرد عليها غامر من النمط- YJ

Quasi Duo Rings whose Every Simple Singular Modules is YJ-Injective حلقات كوازي ديو والتي كل مقاس بسيط منفرد عليها غامر من النمط- YJ Quasi Duo Rings whose Every Simple Singular Modules is YJ-Injective Akram S. Mohammed 1*, Sinan O. AL-Salihi 1 Department of Mathematics,College of Computer Science and Mathematics,University of Tikrit,

More information

Salmon: Lectures on partial differential equations

Salmon: Lectures on partial differential equations 4 Burger s equation In Lecture 2 we remarked that if the coefficients in u x, y,! "! "x + v x,y,! "! "y = 0 depend not only on x,y but also on!, then the characteristics may cross and the solutions become

More information

Compound Damped Pendulum: An Example

Compound Damped Pendulum: An Example Compound Damped Pendulum: An Example Temple H. Fay Department of Mathematical Technology 1 Tshwane University of Technology Pretoria, South Africa thf ay@hotmail:com Abstract: In this article, we use an

More information

Modified Simple Equation Method and its Applications for some Nonlinear Evolution Equations in Mathematical Physics

Modified Simple Equation Method and its Applications for some Nonlinear Evolution Equations in Mathematical Physics Modified Simple Equation Method and its Applications for some Nonlinear Evolution Equations in Mathematical Physics Elsayed M. E. Zayed Mathematics department, Faculty of Science Zagazig University, Zagazig,

More information

The measurements of neutron Fermi Age for selected Nuclear Reactor. shielding materials using the Indium foil technique

The measurements of neutron Fermi Age for selected Nuclear Reactor. shielding materials using the Indium foil technique Iraqi Journal of Physics, 2013 Vol.11, No.22, PP. 27-32 The measurements of neutron Fermi Age for selected Nuclear Reactor Abstract shielding materials using the Indium foil technique Mahdi Hadi Jasim,

More information

Rational Energy Balance Method to Nonlinear Oscillators with Cubic Term

Rational Energy Balance Method to Nonlinear Oscillators with Cubic Term From the SelectedWorks of Hassan Askari 2013 Rational Energy Balance Method to Nonlinear Oscillators with Cubic Term Hassan Askari Available at: https://works.bepress.com/hassan_askari/4/ Asian-European

More information

Cherry Creek High School Summer Assignment for students entering: Accelerated CP Geometry

Cherry Creek High School Summer Assignment for students entering: Accelerated CP Geometry Cherry Creek High School Summer Assignment for students entering: Accelerated CP Geometry Please have the following worksheets completed and ready to be handed in on the first day of class in the fall.

More information

Solving PDEs with Multigrid Methods p.1

Solving PDEs with Multigrid Methods p.1 Solving PDEs with Multigrid Methods Scott MacLachlan maclachl@colorado.edu Department of Applied Mathematics, University of Colorado at Boulder Solving PDEs with Multigrid Methods p.1 Support and Collaboration

More information

Chapter 1. Introduction to Nonlinear Space Plasma Physics

Chapter 1. Introduction to Nonlinear Space Plasma Physics Chapter 1. Introduction to Nonlinear Space Plasma Physics The goal of this course, Nonlinear Space Plasma Physics, is to explore the formation, evolution, propagation, and characteristics of the large

More information

Fluid Mechanics Theory I

Fluid Mechanics Theory I Fluid Mechanics Theory I Last Class: 1. Introduction 2. MicroTAS or Lab on a Chip 3. Microfluidics Length Scale 4. Fundamentals 5. Different Aspects of Microfluidcs Today s Contents: 1. Introduction to

More information

Math Analysis Notes Mrs. Atkinson 1

Math Analysis Notes Mrs. Atkinson 1 Name: Math Analysis Chapter 7 Notes Day 6: Section 7-1 Solving Systems of Equations with Two Variables; Sections 7-1: Solving Systems of Equations with Two Variables Solving Systems of equations with two

More information

Chapter 2 Linear Equations and Inequalities in One Variable

Chapter 2 Linear Equations and Inequalities in One Variable Chapter 2 Linear Equations and Inequalities in One Variable Section 2.1: Linear Equations in One Variable Section 2.3: Solving Formulas Section 2.5: Linear Inequalities in One Variable Section 2.6: Compound

More information

CHAPTER 4. Introduction to the. Heat Conduction Model

CHAPTER 4. Introduction to the. Heat Conduction Model A SERIES OF CLASS NOTES FOR 005-006 TO INTRODUCE LINEAR AND NONLINEAR PROBLEMS TO ENGINEERS, SCIENTISTS, AND APPLIED MATHEMATICIANS DE CLASS NOTES 4 A COLLECTION OF HANDOUTS ON PARTIAL DIFFERENTIAL EQUATIONS

More information

COMPLEX SOLUTIONS FOR TSUNAMI-ASCENDING INTO A RIVER AS A BORE

COMPLEX SOLUTIONS FOR TSUNAMI-ASCENDING INTO A RIVER AS A BORE Volume 114 No. 6 2017, 99-107 ISSN: 1311-8080 (printed version); ISSN: 1314-3395 (on-line version) url: http://www.ijpam.eu ijpam.eu COMPLEX SOLUTIONS FOR TSUNAMI-ASCENDING INTO A RIVER AS A BORE V. Yuvaraj

More information

A linear equation in two variables is generally written as follows equation in three variables can be written as

A linear equation in two variables is generally written as follows equation in three variables can be written as System of Equations A system of equations is a set of equations considered simultaneously. In this course, we will discuss systems of equation in two or three variables either linear or quadratic or a

More information

A Study of the Variational Iteration Method for Solving. Three Species Food Web Model

A Study of the Variational Iteration Method for Solving. Three Species Food Web Model Int. Journal of Math. Analysis, Vol. 6, 2012, no. 16, 753-759 A Study of the Variational Iteration Method for Solving Three Species Food Web Model D. Venu Gopala Rao Home: Plot No.159, Sector-12, M.V.P.Colony,

More information

Bernstein operational matrices for solving multiterm variable order fractional differential equations

Bernstein operational matrices for solving multiterm variable order fractional differential equations International Journal of Current Engineering and Technology E-ISSN 2277 4106 P-ISSN 2347 5161 2017 INPRESSCO All Rights Reserved Available at http://inpressco.com/category/ijcet Research Article Bernstein

More information

Variational Iteration Method for a Class of Nonlinear Differential Equations

Variational Iteration Method for a Class of Nonlinear Differential Equations Int J Contemp Math Sciences, Vol 5, 21, no 37, 1819-1826 Variational Iteration Method for a Class of Nonlinear Differential Equations Onur Kıymaz Ahi Evran Uni, Dept of Mathematics, 42 Kırşehir, Turkey

More information

Conservation Laws and Finite Volume Methods

Conservation Laws and Finite Volume Methods Conservation Laws and Finite Volume Methods AMath 574 Winter Quarter, 2011 Randall J. LeVeque Applied Mathematics University of Washington January 3, 2011 R.J. LeVeque, University of Washington AMath 574,

More information

An explicit exponential finite difference method for the Burgers equation

An explicit exponential finite difference method for the Burgers equation European International Journal of Science and Technology Vol. 2 No. 10 December, 2013 An explicit exponential finite difference method for the Burgers equation BİLGE İNAN*, AHMET REFİK BAHADIR Department

More information

EXPERIENCE COLLEGE BEFORE COLLEGE

EXPERIENCE COLLEGE BEFORE COLLEGE Mechanics, Heat, and Sound (PHY302K) College Unit Week Dates Big Ideas Subject Learning Outcomes Assessments Apply algebra, vectors, and trigonometry in context. Employ units in problems. Course Mathematics

More information

Benha University Faculty of Science Department of Mathematics. (Curriculum Vitae)

Benha University Faculty of Science Department of Mathematics. (Curriculum Vitae) Benha University Faculty of Science Department of Mathematics (Curriculum Vitae) (1) General *Name : Mohamed Meabed Bayuomi Khader *Date of Birth : 24 May 1973 *Marital Status: Married *Nationality : Egyptian

More information

Research Article On the Numerical Solution of Differential-Algebraic Equations with Hessenberg Index-3

Research Article On the Numerical Solution of Differential-Algebraic Equations with Hessenberg Index-3 Discrete Dynamics in Nature and Society Volume, Article ID 474, pages doi:.55//474 Research Article On the Numerical Solution of Differential-Algebraic Equations with Hessenberg Inde- Melike Karta and

More information

Study of Actual Jupiter Observation Days at UFRO Station During 2004 Year دراسة أيام مشاهدات المشتري الفعلية على محطة افرو خالل سنة 4002

Study of Actual Jupiter Observation Days at UFRO Station During 2004 Year دراسة أيام مشاهدات المشتري الفعلية على محطة افرو خالل سنة 4002 Study of Actual Jupiter Observation s at UFRO Station During 2004 Year Kamal M. Abood, Hiba U. Alaa-AlDeen * Department of Astronomy and Space, College of Science, University of Baghdad, Baghdad, Iraq

More information

4. The Green Kubo Relations

4. The Green Kubo Relations 4. The Green Kubo Relations 4.1 The Langevin Equation In 1828 the botanist Robert Brown observed the motion of pollen grains suspended in a fluid. Although the system was allowed to come to equilibrium,

More information

UNSTEADY MHD FLOW OF A VISCOELASTIC FLUID WITH THE FRACTIONAL BURGERS' MODEL

UNSTEADY MHD FLOW OF A VISCOELASTIC FLUID WITH THE FRACTIONAL BURGERS' MODEL UNSTEADY MHD FLOW OF A VISCOELASTIC FLUID WITH THE FRACTIONAL BURGERS' MODEL Ahmad M.Abdul Hadi Departement of Mathematics, College of Science, University of Baghdad.Baghdad- Iraq abstract The aim of this

More information

CRANK-NICOLSON FINITE DIFFERENCE METHOD FOR SOLVING TIME-FRACTIONAL DIFFUSION EQUATION

CRANK-NICOLSON FINITE DIFFERENCE METHOD FOR SOLVING TIME-FRACTIONAL DIFFUSION EQUATION Journal of Fractional Calculus and Applications, Vol. 2. Jan. 2012, No. 2, pp. 1-9. ISSN: 2090-5858. http://www.fcaj.webs.com/ CRANK-NICOLSON FINITE DIFFERENCE METHOD FOR SOLVING TIME-FRACTIONAL DIFFUSION

More information

Lecture 12: Transcritical flow over an obstacle

Lecture 12: Transcritical flow over an obstacle Lecture 12: Transcritical flow over an obstacle Lecturer: Roger Grimshaw. Write-up: Erinna Chen June 22, 2009 1 Introduction The flow of a fluid over an obstacle is a classical and fundamental problem

More information

Galerkin method for the numerical solution of the RLW equation using quintic B-splines

Galerkin method for the numerical solution of the RLW equation using quintic B-splines Journal of Computational and Applied Mathematics 19 (26) 532 547 www.elsevier.com/locate/cam Galerkin method for the numerical solution of the RLW equation using quintic B-splines İdris Dağ a,, Bülent

More information

On The Queuing System M/E r /1/N

On The Queuing System M/E r /1/N On The Queuing System M/E //N Namh A. Abid* Azmi. K. Al-Madi** Received 3, Mach, 2 Acceted 8, Octobe, 2 Abstact: In this ae the queuing system (M/E //N) has been consideed in equilibium. The method of

More information

Various lecture notes for

Various lecture notes for Various lecture notes for 18311. R. R. Rosales (MIT, Math. Dept., 2-337) April 12, 2013 Abstract Notes, both complete and/or incomplete, for MIT s 18.311 (Principles of Applied Mathematics). These notes

More information

Studying the spectral properties of thin films of rhodamine (6G) dyes doped polymer (PMMA) dissolved in chloroform المذابة في الكلوروفورم

Studying the spectral properties of thin films of rhodamine (6G) dyes doped polymer (PMMA) dissolved in chloroform المذابة في الكلوروفورم Iraqi Journal of Physics, 2014 Vol.12, No.23, PP. 59-64 Studying the spectral properties of thin films of rhodamine (6G) dyes doped polymer (PMMA) dissolved in chloroform Ali H. Al-Hamdani 1, Rafah Abdul

More information

Prototype Instabilities

Prototype Instabilities Prototype Instabilities David Randall Introduction Broadly speaking, a growing atmospheric disturbance can draw its kinetic energy from two possible sources: the kinetic and available potential energies

More information

One Solution Two Solutions Three Solutions Four Solutions. Since both equations equal y we can set them equal Combine like terms Factor Solve for x

One Solution Two Solutions Three Solutions Four Solutions. Since both equations equal y we can set them equal Combine like terms Factor Solve for x Algebra Notes Quadratic Systems Name: Block: Date: Last class we discussed linear systems. The only possibilities we had we 1 solution, no solution or infinite solutions. With quadratic systems we have

More information

Section 2.1 (First Order) Linear DEs; Method of Integrating Factors. General first order linear DEs Standard Form; y'(t) + p(t) y = g(t)

Section 2.1 (First Order) Linear DEs; Method of Integrating Factors. General first order linear DEs Standard Form; y'(t) + p(t) y = g(t) Section 2.1 (First Order) Linear DEs; Method of Integrating Factors Key Terms/Ideas: General first order linear DEs Standard Form; y'(t) + p(t) y = g(t) Integrating factor; a function μ(t) that transforms

More information

Application of Laplace Adomian Decomposition Method for the soliton solutions of Boussinesq-Burger equations

Application of Laplace Adomian Decomposition Method for the soliton solutions of Boussinesq-Burger equations Int. J. Adv. Appl. Math. and Mech. 3( (05 50 58 (ISSN: 347-59 IJAAMM Journal homepage: www.ijaamm.com International Journal of Advances in Applied Mathematics and Mechanics Application of Laplace Adomian

More information

Some notes about PDEs. -Bill Green Nov. 2015

Some notes about PDEs. -Bill Green Nov. 2015 Some notes about PDEs -Bill Green Nov. 2015 Partial differential equations (PDEs) are all BVPs, with the same issues about specifying boundary conditions etc. Because they are multi-dimensional, they can

More information

Revision notes for Pure 1(9709/12)

Revision notes for Pure 1(9709/12) Revision notes for Pure 1(9709/12) By WaqasSuleman A-Level Teacher Beaconhouse School System Contents 1. Sequence and Series 2. Functions & Quadratics 3. Binomial theorem 4. Coordinate Geometry 5. Trigonometry

More information

R- Annihilator Small Submodules المقاسات الجزئية الصغيرة من النمط تالف R

R- Annihilator Small Submodules المقاسات الجزئية الصغيرة من النمط تالف R ISSN: 0067-2904 R- Annihilator Small Submodules Hala K. Al-Hurmuzy*, Bahar H. Al-Bahrany Department of Mathematics, College of Science, Baghdad University, Baghdad, Iraq Abstract Let R be an associative

More information

A residual method using Bézier curves for singular nonlinear equations of Lane-Emden type

A residual method using Bézier curves for singular nonlinear equations of Lane-Emden type Kuwait 9 J. Sci. A 44 residual (4) pp method 9-18, 2017 using Bézier curves singular nonlinear equations of Lane-Emden type A residual method using Bézier curves singular nonlinear equations of Lane-Emden

More information

VARIED FLOW IN OPEN CHANNELS

VARIED FLOW IN OPEN CHANNELS Chapter 15 Open Channels vs. Closed Conduits VARIED FLOW IN OPEN CHANNELS Fluid Mechanics, Spring Term 2011 In a closed conduit there can be a pressure gradient that drives the flow. An open channel has

More information

Scalar Conservation Laws and First Order Equations Introduction. Consider equations of the form. (1) u t + q(u) x =0, x R, t > 0.

Scalar Conservation Laws and First Order Equations Introduction. Consider equations of the form. (1) u t + q(u) x =0, x R, t > 0. Scalar Conservation Laws and First Order Equations Introduction. Consider equations of the form (1) u t + q(u) x =, x R, t >. In general, u = u(x, t) represents the density or the concentration of a physical

More information

Predicting the future with Newton s Second Law

Predicting the future with Newton s Second Law Predicting the future with Newton s Second Law To represent the motion of an object (ignoring rotations for now), we need three functions x(t), y(t), and z(t), which describe the spatial coordinates of

More information

Classification of partial differential equations and their solution characteristics

Classification of partial differential equations and their solution characteristics 9 TH INDO GERMAN WINTER ACADEMY 2010 Classification of partial differential equations and their solution characteristics By Ankita Bhutani IIT Roorkee Tutors: Prof. V. Buwa Prof. S. V. R. Rao Prof. U.

More information

Higher Tier - Algebra revision

Higher Tier - Algebra revision Higher Tier - Algebra revision Contents: Indices Epanding single brackets Epanding double brackets Substitution Solving equations Solving equations from angle probs Finding nth term of a sequence Simultaneous

More information

A New Technique of Initial Boundary Value Problems. Using Adomian Decomposition Method

A New Technique of Initial Boundary Value Problems. Using Adomian Decomposition Method International Mathematical Forum, Vol. 7, 2012, no. 17, 799 814 A New Technique of Initial Boundary Value Problems Using Adomian Decomposition Method Elaf Jaafar Ali Department of Mathematics, College

More information

6-3 Solving Systems by Elimination

6-3 Solving Systems by Elimination Another method for solving systems of equations is elimination. Like substitution, the goal of elimination is to get one equation that has only one variable. To do this by elimination, you add the two

More information

Solution of Nonlinear Ordinary Delay Differential Equations Using Variational Approach

Solution of Nonlinear Ordinary Delay Differential Equations Using Variational Approach Solution of Nonlinear Ordinary Delay Differential Equations Using Variational Approach Zainab A. Abdullah Department of Mathematics, College of Science for Women, University of Baghdad, Baghdad-Iraq. Abstract

More information

Conservation and dissipation principles for PDEs

Conservation and dissipation principles for PDEs Conservation and dissipation principles for PDEs Modeling through conservation laws The notion of conservation - of number, energy, mass, momentum - is a fundamental principle that can be used to derive

More information

Equations in Quadratic Form

Equations in Quadratic Form Equations in Quadratic Form MATH 101 College Algebra J. Robert Buchanan Department of Mathematics Summer 2012 Objectives In this lesson we will learn to: make substitutions that allow equations to be written

More information

Math 575-Lecture 26. KdV equation. Derivation of KdV

Math 575-Lecture 26. KdV equation. Derivation of KdV Math 575-Lecture 26 KdV equation We look at the KdV equations and the so-called integrable systems. The KdV equation can be written as u t + 3 2 uu x + 1 6 u xxx = 0. The constants 3/2 and 1/6 are not

More information

Lecture 1: Introduction to Linear and Non-Linear Waves

Lecture 1: Introduction to Linear and Non-Linear Waves Lecture 1: Introduction to Linear and Non-Linear Waves Lecturer: Harvey Segur. Write-up: Michael Bates June 15, 2009 1 Introduction to Water Waves 1.1 Motivation and Basic Properties There are many types

More information

Basic Fluid Mechanics

Basic Fluid Mechanics Basic Fluid Mechanics Chapter 5: Application of Bernoulli Equation 4/16/2018 C5: Application of Bernoulli Equation 1 5.1 Introduction In this chapter we will show that the equation of motion of a particle

More information

MATH 308 Differential Equations

MATH 308 Differential Equations MATH 308 Differential Equations Summer, 2014, SET 1 JoungDong Kim Set 1: Section 1.1, 1.2, 1.3, 2.1 Chapter 1. Introduction 1. Why do we study Differential Equation? Many of the principles, or laws, underlying

More information

Lagrange method (non-parametric method of characteristics)

Lagrange method (non-parametric method of characteristics) 1. Lagrange method (non-parametric method of characteristics) The fact that families of curves and surfaces can be defined by a differential equation means that the equation can be studied geometrically

More information

The Method of Substitution. Linear and Nonlinear Systems of Equations. The Method of Substitution. The Method of Substitution. Example 2.

The Method of Substitution. Linear and Nonlinear Systems of Equations. The Method of Substitution. The Method of Substitution. Example 2. The Method of Substitution Linear and Nonlinear Systems of Equations Precalculus 7.1 Here is an example of a system of two equations in two unknowns. Equation 1 x + y = 5 Equation 3x y = 4 A solution of

More information

A Variational Iterative Method for Solving the Linear and Nonlinear Klein-Gordon Equations

A Variational Iterative Method for Solving the Linear and Nonlinear Klein-Gordon Equations Applied Mathematical Sciences, Vol. 4, 21, no. 39, 1931-194 A Variational Iterative Method for Solving the Linear and Nonlinear Klein-Gordon Equations M. Hussain and Majid Khan Department of Sciences and

More information

Grade 8 Curriculum Map Key: Math in Focus Course 1 (MIF)

Grade 8 Curriculum Map Key: Math in Focus Course 1 (MIF) TIME FRAME September (18 days) UNIT/CONCEPT S Course 3A Content Chapter 1: Exponents CORE GOALS & SKILLS Big Idea : You can use exponential notation to represent repeated multiplication of the same factor

More information

Lecture 3 (Limits and Derivatives)

Lecture 3 (Limits and Derivatives) Lecture 3 (Limits and Derivatives) Continuity In the previous lecture we saw that very often the limit of a function as is just. When this is the case we say that is continuous at a. Definition: A function

More information

Dispersion relations, stability and linearization

Dispersion relations, stability and linearization Dispersion relations, stability and linearization 1 Dispersion relations Suppose that u(x, t) is a function with domain { < x 0}, and it satisfies a linear, constant coefficient partial differential

More information

Advection Diffusion Problems with Pure Advection Approximation in Subregions

Advection Diffusion Problems with Pure Advection Approximation in Subregions Advection Diffusion Problems with Pure Advection Approximation in Subregions M. J. Gander, L. Halpern 2, C. Japhet 2, and V. Martin 3 Université de Genève, 2-4 rue du Lièvre, CP 64, CH-2 Genève. Switzerland.

More information

6-4 Solving Special Systems

6-4 Solving Special Systems 6-4 Solving Special Systems Warm Up Lesson Presentation Lesson Quiz 1 2 pts Bell Quiz 6-4 Solve the equation. 1. 2(x + 1) = 2x + 2 3 pts Solve by using any method. 2. y = 3x + 2 2x + y = 7 5 pts possible

More information

Sixth and Fourth Order Compact Finite Difference Schemes for Two and Three Dimension Poisson Equation with Two Methods to derive These Schemes

Sixth and Fourth Order Compact Finite Difference Schemes for Two and Three Dimension Poisson Equation with Two Methods to derive These Schemes Basra Journal of Scienec (A) Vol.(),-0, 00 Sit and Fourt Order Compact Finite Difference Scemes for Two and Tree Dimension Poisson Equation wit Two Metods to derive Tese Scemes Akil J. Harfas Huda A. Jalob

More information

Numerical solution for chemical kinetics system by using efficient iterative method

Numerical solution for chemical kinetics system by using efficient iterative method International Journal of Advanced Scientific and Technical Research Issue 6 volume 1, Jan Feb 2016 Available online on http://wwwrspublicationcom/ijst/indexhtml ISSN 2249-9954 Numerical solution for chemical

More information

Introduction to Aerodynamics. Dr. Guven Aerospace Engineer (P.hD)

Introduction to Aerodynamics. Dr. Guven Aerospace Engineer (P.hD) Introduction to Aerodynamics Dr. Guven Aerospace Engineer (P.hD) Aerodynamic Forces All aerodynamic forces are generated wither through pressure distribution or a shear stress distribution on a body. The

More information

EXACT SOLUTIONS TO THE NAVIER-STOKES EQUATION FOR AN INCOMPRESSIBLE FLOW FROM THE INTERPRETATION OF THE SCHRÖDINGER WAVE FUNCTION

EXACT SOLUTIONS TO THE NAVIER-STOKES EQUATION FOR AN INCOMPRESSIBLE FLOW FROM THE INTERPRETATION OF THE SCHRÖDINGER WAVE FUNCTION EXACT SOLUTIONS TO THE NAVIER-STOKES EQUATION FOR AN INCOMPRESSIBLE FLOW FROM THE INTERPRETATION OF THE SCHRÖDINGER WAVE FUNCTION Vladimir V. KULISH & José L. LAGE School of Mechanical & Aerospace Engineering,

More information

DIFFERENTIATION AND INTEGRATION PART 1. Mr C s IB Standard Notes

DIFFERENTIATION AND INTEGRATION PART 1. Mr C s IB Standard Notes DIFFERENTIATION AND INTEGRATION PART 1 Mr C s IB Standard Notes In this PDF you can find the following: 1. Notation 2. Keywords Make sure you read through everything and the try examples for yourself before

More information

3. Solving wave and wave-like equations by TAM

3. Solving wave and wave-like equations by TAM A Semi-Analytical Iterative Method for Solving Linear and Nonlinear Partial Differential Equations M.A.AL-Jawary 1, Areej Salah Mohammed 2 1,2 Department of mathematics, Baghdad University, College of

More information

Miller Objectives Alignment Math

Miller Objectives Alignment Math Miller Objectives Alignment Math 1050 1 College Algebra Course Objectives Spring Semester 2016 1. Use algebraic methods to solve a variety of problems involving exponential, logarithmic, polynomial, and

More information

Adsorption of Congo, Red Rhodamine B and Disperse Blue Dyes From Aqueous Solution onto Raw Flint Clay

Adsorption of Congo, Red Rhodamine B and Disperse Blue Dyes From Aqueous Solution onto Raw Flint Clay Adsorption of Congo, Red Rhodamine B and Disperse Blue Dyes From Aqueous Solution onto Raw Flint Clay Sameer H. Kareem* Enaas ABD-Al-Hussien* Received 25, October, 2011 Accepted 18, January, 2012 Abstract:

More information