Title: ME%20440%20Intermediate%20Vibrations
1ME 440Intermediate Vibrations
- Spring 2009
- Tu, January 20
Dan NegrutUniversity of Wisconsin, Madison
2Before 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
3ME440
- 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
4Course 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
5Instructor 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
6Good 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
7ME 440 Fall 2009
- Office Hours
- Monday 2 4 PM
- Wednesday 2 4 PM
- Friday 3 4 PM
7
8Text
- 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
9Other 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
10Grading
- 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
11Homework
- 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
12Midterm 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
13Final Exam
- There will be no final exam
- The third exam will be a comprehensive exam
13
14Scores 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
15PrerequisiteME340
15
16MATLAB 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
17ME440 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
18This 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
20Mechanical 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
21Mechanical Vibrations The Framework (Contd)
- Picture worth all the words on previous slide
21
22What 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
23The 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
24Type 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
25Typical 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
26Linear or Nonlinear ODE
26
27How 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
28Vibration, 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
29Springs
- 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
30Spring (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
k stiffness (units N/m or lb/in)
Energy Stored (linear springs)
30
31Springs Dont Necessarily Look Like
SpringsSpring Constants of Common Elements
31
32Example (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
33Springs 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
34Springs 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
35Equivalent Spring Stiffness
- Another way to compute keq draws on a total
potential energy approach
- Example provided in the textbook
35