What are Numerical Methods? (1/3)

Similar documents
CHAPTER 1 INTRODUCTION TO NUMERICAL METHOD

Civil Engineering Computation. Initial Meeting and Class Setup EXCEL Review Problems

Computational Methods for Engineers Programming in Engineering Problem Solving

PY1008 / PY1009 Physics Gravity I

Chapter 9b: Numerical Methods for Calculus and Differential Equations. Initial-Value Problems Euler Method Time-Step Independence MATLAB ODE Solvers

PowerPoints organized by Dr. Michael R. Gustafson II, Duke University

Exploring the Effect of Bungee Length Manipulation on Acceleration Applied to Jumper

Newton s Laws.

THE MAXIMUM VELOCITY OF A FALLING BODY

Lab #7: Energy Conservation

Introduction to First Order Equations Sections

FORCE. Definition: Combining Forces (Resultant Force)

NEWTON S LAWS OF MOTION

Ch 6 Using Newton s Laws. Applications to mass, weight, friction, air resistance, and periodic motion

cha1873x_p02.qxd 3/21/05 1:01 PM Page 104 PART TWO

Predicting the future with Newton s Second Law

Newton s Laws of Motion and Gravitation

Conceptual Physics 11 th Edition

Resistance is Futile

Topic #7: Forces and Free Body Diagrams (Teacher) Defined as: any influence which tends to change the motion of an object.

Chapter 1 Computer Arithmetic

6.1 Simulation of Simple Systems

Boyce/DiPrima 10 th ed, Ch 1.1: Basic Mathematical Models; Direction Fields

Chapter 6 Dynamics I: Motion Along a Line

Newton's second law of motion

Lecture 6.1 Work and Energy During previous lectures we have considered many examples, which can be solved using Newtonian approach, in particular,

MA 102 Mathematics II Lecture Feb, 2015

Differential relations for fluid flow

Numerical Integration and Numerical Differentiation. Hsiao-Lung Chan Dept Electrical Engineering Chang Gung University, Taiwan

What does the lab partner observe during the instant the student pushes off?

Physics for Scientists and Engineers. Chapter 6 Dynamics I: Motion Along a Line

KINEMATICS OF A PARTICLE. Prepared by Engr. John Paul Timola

PHYSICS. Chapter 5 Lecture FOR SCIENTISTS AND ENGINEERS A STRATEGIC APPROACH 4/E RANDALL D. KNIGHT Pearson Education, Inc.

HSC PHYSICS ONLINE B F BA. repulsion between two negatively charged objects. attraction between a negative charge and a positive charge

2.3: Modeling with Differential Equations

PHYSICS. Hence the velocity of the balloon as seen from the car is m/s towards NW.

Physics 1A Lecture 4B. "Fig Newton: The force required to accelerate a fig inches per second. --J. Hart

Lecture Fluid system elements

Experiment 6: Viscosity (Stoke s Law)

PH211 Chapter 4 Solutions

Differential Equations and the Parachute Problem

AP Physics Laboratory #6.1: Analyzing Terminal Velocity Using an Interesting Version of Atwood s Machine

Forces and Motion in One Dimension

Name. VCE Physics Unit 3 Preparation Work

ELASTIC STRINGS & SPRINGS

Physics for Scientists and Engineers. Chapter 5 Force and Motion

Everybody remains in a state of rest or continues to move in a uniform motion, in a straight line, unless acting on by an external force.

Foundations of Physical Science. Unit One: Forces and Motion

2.1 Forces and Free-Body Diagrams

Dynamic Physics for Simulation and Game Programming

ENGI 3424 First Order ODEs Page 1-01

Chapter 4. Forces in One Dimension

Projectile Motion and 2-D Dynamics

2. Mass, Force and Acceleration

Solution of Nonlinear Equations: Graphical and Incremental Sea

Figure 5.1a, b IDENTIFY: Apply to the car. EXECUTE: gives.. EVALUATE: The force required is less than the weight of the car by the factor.

Mon Jan Improved acceleration models: linear and quadratic drag forces. Announcements: Warm-up Exercise:

Non-textbook problem #I: The kinetic energy of a body depends on its mass and speed as. K = 1 2 mv2 (1) m 1 v 2 1 = 1 2 m 2v 2 2 (2)

empirical expressions. The most commonly used expression is F

Forces Part 1: Newton s Laws

PS113 Chapter 4 Forces and Newton s laws of motion

Chapter 5: Forces in Two Dimensions. Click the mouse or press the spacebar to continue.

= 40 N. Q = 60 O m s,k

8. More about calculus in physics

VARIABLE MASS PROBLEMS

Applying Newton s Laws

UNIVERSITY OF SASKATCHEWAN Department of Physics and Engineering Physics

MITOCW free_body_diagrams

UNIT 2: motion, force and energy.

INTRO VIDEO REVIEW QUIZ

F 2 = 26 N.What third force will cause the object to be in equilibrium (acceleration equals zero)?

Forces. Video Demos. Graphing HW: October 03, 2016

It is convenient to think that solutions of differential equations consist of a family of functions (just like indefinite integrals ).

Modeling and Experimentation: Compound Pendulum

SKMM 3023 Applied Numerical Methods

Question 1. G.M. Paily Phys 211

Solution: (a) Before opening the parachute, the differential equation is given by: dv dt. = v. v(0) = 0

Physics 111: Mechanics Lecture 5

Rutgers University Department of Physics & Astronomy. 01:750:271 Honors Physics I Fall Lecture 7 JJ II. Home Page. Title Page.

Chapter 5. Forces in Two Dimensions

Chapter 5 Roots of Equations: Bracketing Models. Gab-Byung Chae

Types of Force. Example. F gravity F friction F applied F air resistance F normal F spring F magnetism F tension. Contact/ Non-Contact

5. Two forces are applied to a 2.0-kilogram block on a frictionless horizontal surface, as shown in the diagram below.

5. All forces change the motion of objects. 6. The net force on an object is equal to the mass of the object times the acceleration of the object.

Chapter 1. Basic Concepts. 1.1 Trajectories

Exam Question 5: Work, Energy, Impacts and Collisions. June 18, Applied Mathematics: Lecture 5. Brendan Williamson.

Computational Fluid Dynamics Prof. Dr. Suman Chakraborty Department of Mechanical Engineering Indian Institute of Technology, Kharagpur

1. A sphere with a radius of 1.7 cm has a volume of: A) m 3 B) m 3 C) m 3 D) 0.11 m 3 E) 21 m 3

2. F = ma. Newton s Laws. 1. Bodies stay at constant velocity unless acted on by outside force!

Name: Ryan Lesher Lab Partner: Brian D Ostroph Section: PHYS Date: 10/31/2017

Lesson 5. Luis Anchordoqui. Physics 168. Tuesday, September 26, 17

UNIVERSITY OF SASKATCHEWAN Department of Physics and Engineering Physics

Asimple spring-loaded toy that jumps up off

CHAPTER 10 GRAVITATION

6.2 Modeling of Systems and Components

5. A balloon of a known mass or weight is dropped from a known height and timed. Determine the average amount of air resistance that acts on it.

AP Physics C: Mechanics 2005 Scoring Guidelines

WS-CH-4 Motion and Force Show all your work and equations used. Isaac Newton ( )

Calculating Acceleration

Physics 103 Newton s 2 nd Law On Atwood s Machine with Computer Based Data Collection

Transcription:

What are Numerical Methods? (1/3) Numerical methods are techniques by which mathematical problems are formulated so that they can be solved by arithmetic and logic operations Because computers excel at performing such operations, numerical methods are sometimes referred to as computer mathematics The role of numerical methods in engineering problem solving has increased dramatically in recent years v v t gm gcd 1 tanh t i cd m i 1 d t v t g 2 vt t t i1 i i i1 c m i

What are Numerical Methods? (2/3) E.g., complicated mathematical problems in speech recognition

What are Numerical Methods? (3/3)

Why Studying Numerical Methods? (1/2) Numerical methods greatly expand the types of problems you can address E.g., handling large systems of equations, nonlinearities, and complicated geometries As such, greatly enhance your problem-solving sills Numerical methods allow you to use canned software packages with insight rather than treating them as black boxes Enable intelligent use of these packages by an understanding the basic theory underlying the methods Many problems cannot be approached using canned programs With the help of numerical methods, you can design your programs to solve problems

Why Studying Numerical Methods? (2/2) Numerical methods are an efficient vehicle for learning to use computers and can also illustrate the power and limitations of computers We should learn to acknowledge and control the errors of approximation that are part and parcel of large-scale numerical methods Numerical methods provide a vehicle for you to reinforce your understanding of mathematics One function of numerical methods is to reduce higher mathematics to basic arithmetic operations. In so doing, we can enhance our understanding and insight of complicated problems

Objectives of this Course This course sets out to introduce the fundamentals underpinning numerical methods Learn to decide how and when to choose a numerical method, and how to implement and apply it to solve practical problems in science and engineering Understand how numerical methods and computers work in tandem to generate reliable solutions to mathematical problems Have a solid appreciation of the capabilities and limitations of various numerical methods

Textbooks Steven C. Chapra, Applied Numerical Methods with MATLAB for Engineers and Scientists, McGraw-Hill, 2012 Steven C. Chapra and Raymond P. Canale, Numerical Methods for Engineers, McGraw-Hill, 2010

Some Numerical Methods (1/2)

Some Numerical Methods (2/2)

Chapter Objectives Provide a concrete idea of what numerical methods are and how they relate to engineering and scientific problem solving Learning how mathematical models can be formulated on the basis of scientific principles to simulate the behavior of a simple physical system Understanding how numerical methods afford a means to generalize solutions in a manner that can be implemented on a digital computer Understanding the different types of conservation laws that lie beneath the models used in the various engineering disciplines and appreciating the difference between steady-state and dynamic solutions of these models Learning about the different types of numerical methods we will cover in this book

A Simple Mathematical Model (1/2) A mathematical model can be broadly defined as a formulation or equation that expresses the essential features of a physical system or process in mathematical terms Models can be represented by a functional relationship between dependent variables, independent variables, parameters, and forcing functions Dependent variable f independent variables, parameters, forcing functions

A Simple Mathematical Model (2/2) Dependent variable - a characteristic that usually reflects the behavior or state of the system Independent variables - dimensions, such as time and space, along which the system s behavior is being determined Parameters - constants reflective of the system s properties or composition Forcing functions - external influences acting upon the system

Modeling: Newton s Second Law of Motion Statement: The time rate of change of momentum of a body is equal to the resultant force acting on it F ma a F m forcing function (net force acting on the object) dependent variable (acceleration ) Parameter (mass of object) No independent variable is involved E.g., it can be used to determine the terminal velocity of a freefalling body near the earth s surface

More on Newton s Second Law of Motion It describes a natural process or system in mathematical terms It represents an idealization and simplification of reality Ignore negligible details of the natural process and focus on its essential manifestations Exclude the effects of relativity that are of minimal importance when applied to object and forces that interact on or about the earth s surface at velocities and on scales visible to humans It yields reproducible results and can be used for predictive purposes Have generalization capabilities

Bungee-Jumping (1/2) For a body falling within the vicinity of the earth, the net force is composed of two opposing forces F F D F U The downward pull of gravity F D The force due to gravity can be formulated as F D mg g is the acceleration due to gravity (9.81m s ) The upward force of air resistance A good approximation is to formulate it as 2 F U FU cdv v is the velocity; c d is the lumped drag coefficient, accounting for the properties of the falling object like shape or surface roughness» The greater the fall velocity, the greater the upward force due to air resistance 2

Bungee-Jumping (2/2) The net force therefore is the difference between downward and upward force. We can a differential equation regarding the velocity of the object dv dt g c d m 2 v v The exact solution of can not be obtained using simple algebraic manipulation but rather using more advanced calculus techniques (when vt 0, t 0 ) vt gm c d tanh gc d m t (an analytical or closed form solution that can exactly satisfy the original differential equation) Here v c t d and tanh t is independent variable, is dependent variable, and m are parameters, g x is the forcing function. x x e e x x e e

Example 1.1 (1/2) A bungee jumper with a mass of 68.1 kg leaps from a stationary hot air balloon (the drag coefficient is 0.25 kg/m) mg c v Compute the velocity for the first 12 s of free fall Determine the terminal velocity that will attained for an infinite long cord d d v gm c 2 v v t t v v gm c d tanh 12 50. 6938 gc m d 68.1 9.80.25 9.8 tanh 0.25 50.6715 t 68.1 t 51.6938 tanh 0.18977t

Example 1.1 (2/2) Using a computer (or a calculator), the model can be used to generate a graphical representation of the system mg v c d gm c d v 2

An example of Numerical Modeling (1/3) Numerical methods are those in which the mathematical problem is reformulated so it can be solved by arithmetic operations E.g., the time rate of change of velocity mentioned earlier: dv dt v t vt i1 vt i t i1 t i (a finite difference approximation of the derivate at time ti) Notice that dv dt lim t0 v t

An example of Numerical Modeling (2/3) Substituting the finite difference into the differential equation gives Solve for dv dt = g c d v(t i+1 ) v(t i ) t i+1 t i m v2 c d = g v(t i ) m 2 c d v(t i+1 ) = v(t i ) + g v(t i ) m 2 (t i+1 t i ) new = old + slope step This approach is formally called Euler s method

An example of Numerical Modeling (3/3) Applying Euler's method in 2 s intervals yields: How do we improve the solution? Smaller steps

Conservation laws (1/3) Conservation laws provide the foundation for many model functions They boil down Change increases decreases Can be used to predict changes with respect to time by given it a special name the time-variable (or transient) computation If no change occurs, the increases and decreases must be in balance Change 0 increases decreases It is given a special name, the steady-state calculation

Conservation laws (2/3) Example: Fluid Flow For steady-state incompressible fluid flow in pipes Flow in Flow out The flow out of the fourth pipe must be 60

Conservation laws (2/2) Different fields of engineering and science apply these laws to different paradigms within the field Among these laws are Conservation of mass Conservation of momentum Conservation of charge Conservation of energy

Summary of Numerical Methods (1/5) The book is divided into five categories of numerical methods Root Finding: Search for the zero of a function Optimization: Determine a value or values of an independent variable that correspond to a best or optimal value of a function

Summary of Numerical Methods (2/5) Linear Algebraic Equations: have to do with finding a set of values that simultaneously satisfy a set of linear algebraic equations

Summary of Numerical Methods (3/5) Curve Fitting Regression: derive a single curve that represents the general trend of the data without necessarily matching any individual points Is usually employed where there is significant degree of error associated with the data Interpolation: determine intermediate values between relatively error-free data points So as to generate tabulated information

Summary of Numerical Methods (4/5) Integration: determine the area under a curve Differentiation: determine a function s slope or its rate of change

Summary of Numerical Methods (5/5) Differential Equation: many physical laws are couched in terms of the rate of change of a quantity (rather than the magnitude of the quantity) which can be represented as differential equations E.g., the acceleration of a falling body (bungee jumper)