ME%20440%20Intermediate%20Vibrations - PowerPoint PPT Presentation

About This Presentation
Title:

ME%20440%20Intermediate%20Vibrations

Description:

The purpose of the course is to develop the skills needed to design ... Paperback international edition available for $35 ($150 for hardcover) 8. Other Tidbits ... – PowerPoint PPT presentation

Number of Views:197
Avg rating:3.0/5.0
Slides: 36
Provided by: darrylg
Learn more at: http://sbel.wisc.edu
Category:

less

Transcript and Presenter's Notes

Title: ME%20440%20Intermediate%20Vibrations


1
ME 440Intermediate Vibrations
  • Spring 2009
  • Tu, January 20

Dan NegrutUniversity of Wisconsin, Madison
2
Before we get started
  • Today
  • ME440 Logistics
  • Syllabus
  • Grading scheme
  • Start Chapter 1, Fundamentals of Vibrations
  • HW Assigned 1.79
  • HW due in one week

2
3
ME440
  • Course Objective
  • The purpose of the course is to develop the
    skills needed to design and analyze mechanical
    systems in which vibration problems are typically
    encountered. These skills include analytical and
    numerical techniques that allow the student to
    model the system, analyze the system performance
    and employ the necessary design changes. Emphasis
    is placed on developing a thorough understanding
    of how the changes in system parameters affect
    the system response.
  • Catalog Description
  • Analytical methods for solution of typical
    vibratory and balancing problems encountered in
    engines and other mechanical systems. Special
    emphasis on dampers and absorbers.

3
4
Course Outcomes
  • Students must have the ability to
  • 1. Derive the equations of motion of single and
    multi-degree of freedom systems, using Newton's
    Laws and energy methods.
  • 2. Determine the natural frequencies and mode
    shapes of single and multi-degree of freedom
    systems.
  • 3. Evaluate the dynamic response of single and
    multi-degree of freedom systems under impulse
    loadings, harmonic loadings, and general periodic
    excitation.
  • 4. Apply modal analysis and orthogonality
    conditions to establish the dynamic
    characteristics of multi-degree of freedom
    systems.
  • 5. Generate finite element models of discrete
    systems to simulate the dynamic response to
    initial conditions and external excitations.

4
5
Instructor Dan Negrut
  • Polytechnic Institute of Bucharest, Romania
  • B.S. Aerospace Engineering (1992)
  • The University of Iowa, Iowa-City
  • Ph.D. Mechanical Engineering (1998)
  • MSC.Software, Ann Arbor, MI
  • Product Development Engineer 1998-2005
  • The University of Michigan
  • Adjunct Assistant Professor, Dept. of Mathematics
    (2004)
  • Division of Mathematics and Computer Science,
    Argonne National Laboratory
  • Visiting Scientist 2004-2005, 2006
  • The University of Wisconsin-Madison, Joined in
    Nov. 2005
  • Research Computer Aided Engineering (tech. lead,
    Simulation-Based Engineering Lab)
  • Focus Computational Dynamics (http//sbel.wisc.ed
    u)

5
6
Good to know
  • Time 930-1045 AM
  • Location
  • 3349EH (through end of Jan)
  • 3126ME (after Feb. 1)
  • Office 2035ME
  • Phone 608 890-0914
  • E-Mail negrut_at_engr.wisc.edu
  • Grader Naresh Khude, khude_at_wisc.edu

6
7
ME 440 Fall 2009
  • Office Hours
  • Monday 2 4 PM
  • Wednesday 2 4 PM
  • Friday 3 4 PM

7
8
Text
  • S. S. Rao Mechanical Vibrations
  • Pearson Prentice Hall
  • Fourth edition (2004)
  • Well cover material out of first six chapters
  • On a couple of occasions, the material in the
    book will be supplemented with notes
  • Available at Wendt Library (on reserve)
  • Paperback international edition available for 35
    (150 for hardcover)

8
9
Other Tidbits
  • Handouts will be printed out and provided before
    each lecture
  • Good idea to organize material provided in a
    folder
  • Useful for PhD Qualifying exam, useful in
    industry
  • Lecture slides will be made available online
  • http//sbel.wisc.edu/Courses/ME440/2009/index.htm
  • Im in the process of reorganizing the class
    material
  • Moving from transparency to slide format
  • Grades will be maintained online at
    https//LearnUW.wisc.edu
  • Schedule will be updated as we go and will
    contain info about
  • Topics we cover
  • Homework assignments

9
10
Grading
  • Homework Projects 40
  • Exam 1 (Feb. 24) 20
  • Exam 2 (Apr. 7) 20
  • Exam 3 (May 7) 20
  • Total 100
  • NOTE
  • Score related questions (homeworks/exams/projects)
    must be raised prior to next class after the
    homeworks/exams/project is returned.
  • Exam 3 will serve as the final exam and it will
    be comprehensive

10
11
Homework
  • Weekly if not daily homework
  • Assigned at the end of each class
  • Due at the beginning of the class, one week later
  • No late homework accepted
  • Two lowest score homeworks will be dropped
  • Grading
  • Each problem scored on a 1-10 scale (10 best)
  • For each HW an average will be computed on a 1-10
    scale
  • Solutions to select problems will be posted at
    Learn_at_UW

11
12
Midterm Exams
  • Scheduled dates on syllabus
  • Tu, 02/24 covers chapters 1 through 3
  • Tu, 04/07 covers chapter 4 through 5
  • Th, 05/07 comprehensive, chapters 1 through 6
  • A review session will be offered prior to each
    exam
  • One day prior to the exam, at 715PM
  • Will run about two hours long
  • Room 3126ME

12
13
Final Exam
  • There will be no final exam
  • The third exam will be a comprehensive exam

13
14
Scores and Grades
Score Grade 94-100 A 87-93 AB 80-86 B 73-79 BC
66-72 C 55-65 D lt54 F
  • Grading will not be done on a curve
  • Final score will be rounded to the nearest
    integer prior to having a letter assigned
  • 86.59 becomes AB
  • 86.47 becomes B

14
15
PrerequisiteME340
15
16
MATLAB and Simulink
  • Integrated into every chapter in the text
  • You are responsible for brushing up on your
    MATLAB skills
  • Ill offer a MATLAB Workshop (outside class)
  • Friday, January 30 1 to 4 PM (room 1051ECB)
  • Topics covered working in MATLAB, working with
    matrices, m-file functions and scripts, for
    loops/while loops, if statements, 2-D plots
  • Actually it covers more than you need to know for
    ME440
  • Offered to ME students, seating is limited,
    register if you plan to attend
  • Resources posted on course website
  • MATLAB workshop tutorial

16
17
ME440 Major Topics
  • Chapter 1 Fundamentals of Vibrations
  • Chapter 2 Free Vibrations of Single DOF Systems
  • Chapter 3 Harmonically Excited Vibration
  • Chapter 4 Vibration Under General Forcing
    Conditions
  • Chapter 5 Two Degree of Freedom Systems
  • Chapter 6 Multidegree of Freedom Systems

17
18
This Course
  • Be active, pay attention, ask questions
  • A rather intense class
  • The most important thing is taking care of
    homework
  • Reading the text is important
  • The class builds on itself essential to start
    strong and keep up
  • Your feedback is important
  • Provide feedback both during and at end of the
    semester

18
19
  • End ME440 Logistics, Syllabus Discussion
  • Begin Chapter 1 - Fundamentals of Vibration

19
20
Mechanical Vibrations The Framework
  • How has this topic, Mechanical Vibrations, come
    to be?
  • Just like many other topics in Engineering
  • A physical system is given to you (you have a
    problem to solve)
  • You generate an abstraction of that actual system
    (problem)
  • In other words, you generate a model of the
    system
  • You apply the laws of physics to get the
    equations that govern the time evolution of the
    model
  • You solve the differential equations to find the
    solution of interest
  • Post-processing might be necessary

20
21
Mechanical Vibrations The Framework (Contd)
  • Picture worth all the words on previous slide

21
22
What is the problem here?
  • Both the mass-spring-damper system and the string
    system lead to an oscillatory motion
  • Vibration, Oscillation
  • Any motion that repeats itself after in interval
    of time
  • For the mass-spring-damper
  • One degree of freedom system
  • Everything is settled once you get the solution
    x(t)
  • You get x(t) as the solution of an Initial Value
    Problem (IVP)
  • For the string
  • An infinite number of degrees of freedom
  • You need the string deflection at each location x
    between 0 and L
  • You get the string deflection as a function of
    time and location based on both initial
    conditions and boundary conditions solution of
    a set of Partial Differential Equations

22
23
The Concept of Degree of Freedom
  • Degree of Freedom
  • This concept means different things to different
    people
  • In ME440
  • The minimum number of coordinates (states,
    unknowns, etc.) that you need to have in your
    model to uniquely specify the position/orientation
    of each component in your model

23
24
Type of Math Problems in Vibrations
  • Two different problems lead to two different
    models
  • Lumped systems lead to ODEs
  • Continuous systems leads to PDEs
  • PDEs are significantly more difficult to solve
  • In this class, well almost exclusively deal with
    systems that lead to ODE problems (lumped
    systems, discrete systems)
  • See next slide

24
25
Typical ME440 Problem
  • Not only that we are going to mostly deal with
    ODEs, but they are typically linear
  • Nonlinear ODEs are most of the time impossible to
    solve in close form
  • You end up using a numerical algorithm to find an
    approximate solution
  • Well work in the blue boxes

25
26
Linear or Nonlinear ODE
26
27
How Things Happen
  • In a oscillatory motion, one type of energy gets
    converted into a different type of energy time
    and again
  • Think of a pendulum
  • Potential energy gets converted into kinetic
    energy which gets connected back into potential
    energy, etc.
  • Note that energy dissipation almost always
    occurs, so the oscillatory motion is damped
  • Air resistance, heat dissipation due to friction,
    etc.

27
28
Vibration, the Characters in the Play
  • One needs elements capable of storing/dissipating
    various forms of energy
  • Springs capable of storing potential energy
  • Masses capable of acquiring kinetic energy
  • Damping elements involved in the energy
    dissipation
  • Actuators the elements that apply an external
    forcing or impose a prescribed motion on parts of
    a system
  • NOTE The systems (problems) that well analyze
    in 440 lead to models based on a combination of
    these four elements

28
29
Springs
  • A component/system that relates a displacement to
    a force that is required to produce that
    displacement
  • Physically, its often times a mechanical link
    typically assumed to have negligible mass and
    damping
  • Well work most of the time with linear springs
  • NOTE After reaching the yield point A, even a
    linear spring stops behaving linearly

29
30
Spring (Stiffness) Element
  • F is the force exerted by the spring
  • x1, x2 are the displacements of spring end
    points
  • Spring deflection ?x x2-x1

x1
x2
F
F
  • Linear springs

k stiffness (units N/m or lb/in)
Energy Stored (linear springs)
30
31
Springs Dont Necessarily Look Like
SpringsSpring Constants of Common Elements
31
32
Example (Equivalent Spring)
  • Assume that mass of beam is negligible in
    comparison with end mass.
  • Denote by Wmg weight of the end mass
  • Static deflection of the cantilever beam is given
    by
  • The equivalent spring has the stiffness

32
33
Springs Acting in Series
F
Note that two springs are in series when a) They
are experiencing the same tension (or
compression) b) Youd add up the deformations to
get the total deformation x
Exercise Show that the equivalent spring
constant keq is such that
The idea is that you want to determine one
abstract spring that has keq that deforms by the
same amount when its subject to F.
33
34
Springs Acting in Parallel
F
F
Note that two springs are in parallel when a)
They experience the same amount of deformation b)
Youd add up the force experienced by each spring
to come up with the total force F
Exercise Show that the equivalent spring
constant keq is such that
34
35
Equivalent Spring Stiffness
  • Another way to compute keq draws on a total
    potential energy approach
  • Example provided in the textbook

35
Write a Comment
User Comments (0)
About PowerShow.com