EG 10111/10112 Introduction to Engineering Copyright © 2009 University of Notre Dame Introduction to Engineering Systems Lecture 3 (9/4/2009) Empirical.

Slides:



Advertisements
Similar presentations
Review: Newton’s 1 st & 2 nd Laws 1 st law (Galileo’s principle of inertia)- no force is needed to keep an object moving with constant velocity 2 nd law.
Advertisements

EG 10111/10112 Introduction to Engineering Copyright © 2009 University of Notre Dame Probability and Limit States Introduction to Engineering Systems Lecture.
Momentum and Impulse. What is Momentum? Momentum – The product of the mass and velocity of an object. Has magnitude and direction. Momentum = p = mv P.
You are given two carts, A and B. They look identical, and you are told that they are made of the same material. You place A at rest on an air track and.
Example: An eagle of mass, mA = 6. 0 kg moving with speed vA = 5
Conservation of Momentum
Law of Conservation of Momentum and Collisions Chapter
1 Chapter Six: Momentum and Collisions. 2 Momentum is the product of the mass of a body and its velocity. A body may be an assembly of particles. Such.
Physics 101: Lecture 12, Pg 1 Physics 101: Lecture 12 Collisions and Explosions l Today’s lecture will cover Textbook Sections Exam II.
EG 10111/10112 Introduction to Engineering Copyright © 2009 University of Notre Dame Line fitting, Hooke’s Law, and Physics of Towers Introduction to Engineering.
EG 10111/10112 Introduction to Engineering Copyright © 2009 University of Notre Dame Technical Communication: Written documents Introduction to Engineering.
EG 10111/10112 Introduction to Engineering Copyright © 2009 University of Notre Dame Exam review (continued) Introduction to Engineering Systems Lecture.
EG 10111/10112 Introduction to Engineering Copyright © 2009 University of Notre Dame Introduction to Engineering Systems Lecture 2 (8/31/2009) Using “Laws.
EG 10111/10112 Introduction to Engineering Copyright © 2009 University of Notre Dame Design optimization: optimization problem and factor of safety (F.O.S.)
EG 10111/10112 Introduction to Engineering Copyright © 2009 University of Notre Dame Statistics and Probability: Betting on a Design Introduction to Engineering.
EG 10111/10112 Introduction to Engineering Copyright © 2009 University of Notre Dame Exam review Introduction to Engineering Systems Lecture 11 (10/02/2009)
AP Physics Review Ch 7 – Impulse and Momentum
Elastic Collisions. Conservation  Elastic collisions conserve both momentum and kinetic energy.  Two equations govern all elastic collisions. m1m1 m2m2.
ENGR 215 ~ Dynamics Sections Central Impact.
ENGR 215 ~ Dynamics Sections Impulse and Linear Momentum In this section we will integrate the equation of motion with respect to time and.
Phy 211: General Physics I Chapter 9: Center of Mass & Linear Momentum Lecture Notes.
Physics 101: Lecture 14, Pg 1 Physics 101: Lecture 14 Impulse and Momentum l Today’s lecture will cover Chapter
Linear Impulse & Linear Momentum
Section 73 Momentum.
Chapter 7: Momentum & Impulse Lecture Notes
Fri. Feb. 25th1 PHSX213 class Class stuff –Questions ? Conservation of Linear Momentum Collision terminology Collisions.
Elastic and Inelastic Collisions Unit A: Momentum.
Dynamics of Moving Objects in Kinetic Sculpture (Ball Drop Physics II)
Newton’s Third Law of Motion
Conservation of Momentum. Conserved Total momentum of a system before and after an interaction remains constant Momentum before = Momentum After Two balls.
Momentum Chapter 6. Momentum ► Related to inertia, not the same. ► Symbol is p ► p=mv ► Units of kgm/s ► What is the momentum of a 75kg rock rolling at.
Momentum, Impulse, and Collisions
Physics 215 – Fall 2014Lecture Welcome back to Physics 215 Today’s agenda: More on momentum, collisions Kinetic and potential energy Potential energy.
Momentum and Its Conservation
LAW OF CONSERVATION OF MOMENTUM
Newton’s Third law and the Conservation of Linear Momentum Syllabus statements due Friday (1/13)
Physics 321 Hour 1 Course Introduction. Course Components Course Outline Prerequisites: ODEs, Mathematica Reading: Due before lecture HW: Due MWF - see.
CMPS 1371 Introduction to Computing for Engineers PRINCIPLES OF PROBLEM SOLVING.
CHAPTER 4 AN INTRODUCTION TO BIOMECHANICS. Biomechanics Biomechanics is the study of how and why the human body moves. Biomechanics is the study of how.
Chapter 9 - Collisions Momentum and force Conservation of momentum
The product of mass and velocity of a body is called momentum. Force and Laws of Motion Momentum Mathematically, Momentum = mass × velocity P = mv It is.
Physics 218 Lecture 15: Momentum Alexei Safonov.
CH01-4 Momentum. Force and momentum A constant force acts on a fan cart. If we double the mass of the cart (with the same force acting on the cart), has.
Momentum and Impulse. March 24, 2009 Momentum and Momentum Conservation  Momentum  Impulse  Conservation of Momentum  Collision in 1-D  Collision.
What is energy? Ability to do work or cause change –Work: ability to move an object some distance.
Momentum Introduction Section 0 Lecture 1 Slide 1 Lecture 15 Slide 1 INTRODUCTION TO Modern Physics PHYX 2710 Fall 2004 Physics of Technology—PHYS 1800.
Physics 101: Lecture 12, Pg 1 Physics 101: Lecture 12 2D Collisions and Center of mass.
Conservation of Momentum. Momentum  The velocity and mass of an object give it momentum.  The larger the velocity and mass, the larger the momentum.
Review: Newton’s 1 st & 2 nd Laws 1 st law (Galileo’s principle of inertia)- no force is needed to keep an object moving with constant velocity 2 nd law.
P69.
Conservation of Momentum. For a collision occurring between two objects in an isolated system, the total momentum of the two objects before the collision.
Chapter 6 Section 2. Objectives  Describe the interaction between two objects in terms of the change in momentum of each object.  Compare the total.
Sect. 9.2: Impulse & Momentum
PHY 101: Lecture The Impulse-Momentum Theorem 7.2 The Principle of Conservation of Linear Momentum 7.3 Collision in One Dimension 7.4 Collisions.
< initial velocity of Object B > initial velocity of Object B
Matt Elder Jessa Meyers Ryan Lewis Michael Love
Different kinds of energy
11.5 Forces.
What is Momentum? Unit 8 Section 3
Momentum:.
Quiz 1 Period 2.
Elastic Collisions.
Elastic Collisions SPH4U.
Momentum “Keep Goingness” of an object. p = mv where p = momentum
Momentum and Impulse HMH Physics Chapter 6 pages
MOMENTUM (p) is defined as the product of the mass and velocity -is based on Newton’s 2nd Law F = m a F = m Δv t F t = m Δv IMPULSE MOMENTUM.
Semester Review Jeopardy.
Ch. 6 Momentum and Impulse
Collisions Chapter 4.
Chapter 9: Center of Mass & Linear Momentum Lecture Notes
Presentation transcript:

EG 10111/10112 Introduction to Engineering Copyright © 2009 University of Notre Dame Introduction to Engineering Systems Lecture 3 (9/4/2009) Empirical Models: Fitting a Line to Experimental Data Prof. Andrés Tovar

EG 10111/10112 Introduction to Engineering Copyright © 2009 University of Notre Dame Reading material and videos LC1 – Measure: Concourse material LT1 – Introduction: Sec. 1.1, 1.2, and 1.4 LT2 – Models: Ch. 4 LC2 – Matlab: Ch. 9 and 10, videos 1 to 9 LT3 – Data analysis: Sec. 5.1 to 5.3, videos 13 and 14 For next week LT4 – Statistics: Sec and 5.4.2, video 10 LC3 – SAP Model: Concourse material LT5 – Probability: Sec and 5.4.4, videos 11 and 12 LT: lecture session LC: learning center session Using "Laws of Nature" to Model a System

EG 10111/10112 Introduction to Engineering Copyright © 2009 University of Notre Dame Announcements Homework 1 –Available on Concourse –Due next week at the beginning of the Learning Center session. Learning Center –Do not bring earphones/headphones. –Do not bring your laptop. –Print and read the material before the session. Using "Laws of Nature" to Model a System

EG 10111/10112 Introduction to Engineering Copyright © 2009 University of Notre Dame From last class The 4 M paradigm: measure, model, modify, and make. Empirical models vs. Theoretical models Models for a falling object –Aristotle (Greece, 384 BC – 322 BC) –Galileo (Italy, 1564 – 1642) –Newton (England, 1643 – 1727) –Leibniz (Germany, 1646 –1716) Models for colliding objects –Descartes (France, ) –Huygens (Deutschland, 1629 – 1695) –Newton (England, 1643 – 1727) Prediction based on models Empirical Models: Fitting a Line to Experimental Data pool ball golf ball

EG 10111/10112 Introduction to Engineering Copyright © 2009 University of Notre Dame From last class Given 2 pendulums with different masses, initially at rest –Say, a golf ball and a pool ball Would you be willing to bet that you could figure out where to release the larger ball in order to knock the smaller ball to a given height? How could you improve your chances? pool ball golf ball Empirical Models: Fitting a Line to Experimental Data

EG 10111/10112 Introduction to Engineering Copyright © 2009 University of Notre Dame Theoretical Model of Colliding Pendulums Given 2 pendulum masses m 1 and m 2 –golf ball initially at h 2i = 0 –pool ball released from h 1i –golf ball bounces up to h 2f –pool ball continues up to h 1f Galileo’s relationship between height and speed later developed by Newton and Leibniz. Huygens’ principle of relative velocity Newton’s “patched up” version of Descartes’ conservation of motion—conservation of momentum Empirical Models: Fitting a Line to Experimental Data pool ball golf ball

EG 10111/10112 Introduction to Engineering Copyright © 2009 University of Notre Dame Theoretical Model of Colliding Pendulums Empirical Models: Fitting a Line to Experimental Data Collision model: Relative velocity Conservation of momentum Conservation of energy

EG 10111/10112 Introduction to Engineering Copyright © 2009 University of Notre Dame Theoretical Model of Colliding Pendulums Empirical Models: Fitting a Line to Experimental Data 1) Conservation of energy 2) Collision model: relative velocity and conservation of momentum 3) Conservation of energy

EG 10111/10112 Introduction to Engineering Copyright © 2009 University of Notre Dame Theoretical Model of Colliding Pendulums Empirical Models: Fitting a Line to Experimental Data 4) Finally 4) In Matlab this is h1i = (h2f*(m1 + m2)^2)/(4*m1^2);

EG 10111/10112 Introduction to Engineering Copyright © 2009 University of Notre Dame Matlab implementation Empirical Models: Fitting a Line to Experimental Data % collision.m m1 = input('Mass of the first (moving) ball m1: '); m2 = input('Mass of the second (static) ball m2: '); h2f = input('Desired final height for the second ball h2f: '); disp('The initial height for the first ball h1i is:') h1i = (h2f*(m1 + m2)^2)/(4*m1^2)

EG 10111/10112 Introduction to Engineering Copyright © 2009 University of Notre Dame Matlab implementation Empirical Models: Fitting a Line to Experimental Data % collision1.m m1 = 0.165; % mass of pool ball, kg m2 = 0.048; % mass of golf ball, kg h2f = input('Desired final height for the second ball h2f: '); disp('The initial height for the first ball h1i is:') h1i = (h2f*(m1 + m2)^2)/(4*m1^2) plot(h2f,h1i,'o'); xlabel('h2f'); ylabel('h1i') hold on Let us compare the theoretical solution with the experimental result. What happened?!?!

EG 10111/10112 Introduction to Engineering Copyright © 2009 University of Notre Dame Run the Pendulum Experiment Empirical Models: Fitting a Line to Experimental Data Pool ball release height (m) Golf ball final height (m)

EG 10111/10112 Introduction to Engineering Copyright © 2009 University of Notre Dame Experimental Results Empirical Models: Fitting a Line to Experimental Data % collision2.m h1ie = 0:0.05:0.25; % heights for pool ball, m h2fe = []; % experimental results for golf ball, m plot(h1ie,h2fe, '*')

EG 10111/10112 Introduction to Engineering Copyright © 2009 University of Notre Dame MATLAB GUI for Least Squares Fit Empirical Models: Fitting a Line to Experimental Data

EG 10111/10112 Introduction to Engineering Copyright © 2009 University of Notre Dame MATLAB commands for Least Squares Fit Empirical Models: Fitting a Line to Experimental Data % collision2.m h1ie = 0:0.05:0.25; % heights for pool ball, m h2fe = []; % experimental results for golf ball, m plot(h1ie,h2fe, '*') c = polyfit(h1ie, h2fe, 1) m = c(1) % slope b = c(2) % intercept h2f = input('Desired final height for the second ball h2f: '); disp('The initial height for the first ball h1i is:') h1i = 1/m*(h2f-b) fit a line (not quadratic, etc)

EG 10111/10112 Introduction to Engineering Copyright © 2009 University of Notre Dame What About Our Theory Is it wrong? Understanding the difference between theory and empirical data leads to a better theory Evolution of theory leads to a better model Empirical Models: Fitting a Line to Experimental Data

EG 10111/10112 Introduction to Engineering Copyright © 2009 University of Notre Dame Improved collision model Empirical Models: Fitting a Line to Experimental Data Huygens’ principle of relative velocity Coefficient of restitution Improved collision model: COR and conservation of momentum hi1 = (h2f*(m1 + m2)^2)/(m1^2*(Cr + 1)^2) The improved theoretical solution is

EG 10111/10112 Introduction to Engineering Copyright © 2009 University of Notre Dame Matlab implementation Empirical Models: Fitting a Line to Experimental Data % collision3.m m1 = 0.165; % mass of pool ball, kg m2 = 0.048; % mass of golf ball, kg Cr = input('Coefficient of restitution: '); h2f = input('Desired final height for the second ball h2f: '); disp('The initial height for the first ball h1i is:') hi1 = (h2f*(m1 + m2)^2)/(m1^2*(Cr + 1)^2) Let us compare the improved theoretical solution with the experimental result. What happened now?