Chapter 1.

Slides:



Advertisements
Similar presentations
ECIV 201 Computational Methods for Civil Engineers Richard P. Ray, Ph.D., P.E. Modeling, Computers, and Error Analysis.
Advertisements

Ch 1.1: Basic Mathematical Models; Direction Fields Differential equations are equations containing derivatives. Derivatives describe rates of change.
Mech300 Numerical Methods, Hong Kong University of Science and Technology. 1 Part Seven Ordinary Differential Equations.
CE 1501 CE 150 Fluid Mechanics G.A. Kallio Dept. of Mechanical Engineering, Mechatronic Engineering & Manufacturing Technology California State University,
ECIV 301 Programming & Graphics Numerical Methods for Engineers Lecture 2 Mathematical Modeling and Engineering Problem Solving.
The Islamic University of Gaza Faculty of Engineering Numerical Analysis ECIV 3306 Introduction.
Numerical Methods for Engineering MECN 3500
Copyright © 2006 The McGraw-Hill Companies, Inc. Permission required for reproduction or display. by Lale Yurttas, Texas A&M University Chapter 11.
Fluid mechanics 3.1 – key points
The Islamic University of Gaza Faculty of Engineering Civil Engineering Department Numerical Analysis ECIV 3306 Chapter 1 Mathematical Modeling.
Copyright © 2006 The McGraw-Hill Companies, Inc. Permission required for reproduction or display. 1 Mathematical Modeling and Engineering Problem solving.
Linear Momentum and Collisions
Newton’s second law of motion
MMJ 1113 Computational Methods for Engineers Mohsin Mohd Sies Fakulti Kejuruteraan Mekanikal, Universiti Teknologi Malaysia.
© Fox, McDonald & Pritchard Introduction to Fluid Mechanics Chapter 5 Introduction to Differential Analysis of Fluid Motion.
Chapter 9: Differential Analysis of Fluid Flow SCHOOL OF BIOPROCESS ENGINEERING, UNIVERSITI MALAYSIA PERLIS.
A PPLIED M ECHANICS Lecture 01 Slovak University of Technology Faculty of Material Science and Technology in Trnava.
Math 3120 Differential Equations with Boundary Value Problems
Chapter Six: Laws of Motion
Mathematical Modeling and Engineering Problem Solving
CSE 3802 / ECE 3431 Numerical Methods in Scientific Computation
Newton’s 2 nd Law of Motion. 2 nd Law Defined The acceleration of an object depends on the mass of the object and the amount of force applied The acceleration.
Honors Physics Newton’s Second Law of Motion.  Newton’s First Law explains the results of zero net external force. –The body stays at rest or moves with.
 Law 1: › Every object in a state of uniform motion tends to remain in that state of motion unless an external force is applied to it.  Law 2 : › The.
Chapter Six: Laws of Motion
Chapter 4 The Laws of Motion. Classical Mechanics Describes the relationship between the motion of objects in our everyday world and the forces acting.
Momentum What is momentum? ~ Newton’s Quality of Motion Use the 2 nd Law…F = ma to describe how momentum can change when a force acts on it. F=ma m ∆v.
ES 240: Scientific and Engineering Computation. Chapter 1 Chapter 1: Mathematical Modeling, Numerical Methods and Problem Solving Uchechukwu Ofoegbu Temple.
Part 1 Chapter 1 Mathematical Modeling, Numerical Methods, and Problem Solving PowerPoints organized by Dr. Michael R. Gustafson II, Duke University and.
Chapter 1: Introduction Note to Students (the points emphasized in syllabus): The classroom time should be used to amplify the text book material by discussing.
© Fox, Pritchard, & McDonald Introduction to Fluid Mechanics Chapter 5 Introduction to Differential Analysis of Fluid Motion.
Dimensional Analysis.
Part 1 Chapter 1 Mathematical Modeling, Numerical Methods, and Problem Solving PowerPoints organized by Dr. Michael R. Gustafson II, Duke University and.
Newton’s Second Law of Motion. 2 nd Law of Motion  The net (total) force of an object is equal to the product of its acceleration and its mass.  Force.
Dr. Wang Xingbo QQ: Homepage: wxbstudio.home4u.china.com Fall , 2005 Mathematical & Mechanical Method in Mechanical.
Engineering Mechanics Statics. Introduction Mechanics - the physical science which describes or predicts the conditions of rest or motion of bodies under.
Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display. 1-1 Chapter 1.
Chapter 1: Basic Concepts
Control engineering ( ) Time response of first order system PREPARED BY: Patel Ravindra.
Solving Engineering Problems
Introduction.
Chapter 4 The Laws of Motion.
Chapter 4 Fluid Mechanics Frank White
Newton’s Second Law of Motion
Physics 210 General Physics I
FLUID DYNAMICS Made By: Prajapati Dharmesh Jyantibhai ( )
Dimensional Analysis.
CE 102 Statics Chapter 1 Introduction.
Introduction.
Selection of A Suitable Branch of Mathematics for Thermofluids
FLUID FLOW TYPICAL ENGINEERING PROBLEMS:
Lesson 52 - Differential Equations
Newton’s Laws Of Motion
Which one would be easier to accelerate by pushing?
Chapter 4 The Laws of Motion.
Solving Engineering Problems
Mathematical Modeling, Numerical Methods, and Problem Solving
Ch 1.1: Basic Mathematical Models; Direction Fields
Introduction.
Ch 1.1: Basic Mathematical Models; Direction Fields
Computational Fluid Dynamics - Fall 2001
Introduction.
MAE 3241: AERODYNAMICS AND FLIGHT MECHANICS
Mathematical Model.
Impulse and Momentum Readings: Chapter 9.
The Laws of Motion (not including Atwood)
SKTN 2393 Numerical Methods for Nuclear Engineers
Newton’s Laws of Motion
Introduction to Fluid Mechanics
Introduction.
Presentation transcript:

Chapter 1

Mathematical Modeling and Engineering Problem solving Chapter 1 Requires understanding of engineering systems By observation and experiment Theoretical analysis and generalization Computers are great tools, however, without fundamental understanding of engineering problems, they will be useless.

Fig. 1.1

Dependent independent forcing A mathematical model is represented as a functional relationship of the form Dependent independent forcing Variable = f variables, parameters, functions Dependent variable: Characteristic that usually reflects the state of the system Independent variables: Dimensions such as time ans space along which the systems behavior is being determined Parameters: reflect the system’s properties or composition Forcing functions: external influences acting upon the system

Newton’s 2nd law of Motion States that “the time rate change of momentum of a body is equal to the resulting force acting on it.” The model is formulated as F = m a (1.2) F=net force acting on the body (N) m=mass of the object (kg) a=its acceleration (m/s2)

Formulation of Newton’s 2nd law has several characteristics that are typical of mathematical models of the physical world: It describes a natural process or system in mathematical terms It represents an idealization and simplification of reality Finally, it yields reproducible results, consequently, can be used for predictive purposes.

Some mathematical models of physical phenomena may be much more complex. Complex models may not be solved exactly or require more sophisticated mathematical techniques than simple algebra for their solution Example, modeling of a falling parachutist:

If the parachutist is initially at rest (v=0 at t=0), using calculus This is a differential equation and is written in terms of the differential rate of change dv/dt of the variable that we are interested in predicting. If the parachutist is initially at rest (v=0 at t=0), using calculus Independent variable Dependent variable Parameters Forcing function

Conservation Laws and Engineering Conservation laws are the most important and fundamental laws that are used in engineering. Change = increases – decreases (1.13) Change implies changes with time (transient). If the change is nonexistent (steady-state), Eq. 1.13 becomes Increases =Decreases

For steady-state incompressible fluid flow in pipes: Fig 1.6 For steady-state incompressible fluid flow in pipes: Flow in = Flow out or 100 + 80 = 120 + Flow4 Flow4 = 60

Refer to Table 1.1