Department
of Mechanical and Materials Engineering
This is the EML 4220 Mechanical Vibrations Fall 2018 page
Here is the EML4220 Syllabus (updated 8/30/18)
We will meet in EC1113 on W from 10-1150am and in EC1113 on F 11-1150am
We will NOT have a TA. If you have any questions come to see me.
My office EC3442 and my telephone number is 305-348-3643; my email levyez@fiu.edu
First Assignment: READ Chapter 1 and Sections 2.1-2.5
in Rao’s book and do the following problems:
Here are problems 1-3, 1-7 and 1-8, 1-9 and 1-10
Here are problems 1-12, 1-13a and 1-13b,
Here are problems 1-29, 1-30, 1-35 and 1-35b
Here are problems 1-53, 1-54, and 1-59
Here is a videotape
on energy
methods and equivalent elements
Even though I will be giving you access to the solutions, you
need to try to do the problems first so that you
will know where you get stuck and then use the solutions to see you get past
the problem. Just looking at the
solutions does not help you understand the methodology in relation to the way
you think about solving the problem. Just as with Dynamics, the only way to
learn vibrations is to do as many problems as you can.
Here are problems 2-4, 2-6 and 2-7 Note that more comments about 2-7
Are found on the top of the page for problem 2-13
Here are problems 2-13 , 2-15. Note that the problem here is LIKE 2-13 in your book
But is not problem 2-13
Please Turn in on
9/5/18 Problems 1-9, 1-10, 2-15 for grading as a
check on learning.
This
material and all the linked materials provided, except where stated
specifically, are copyrighted © Cesar Levy 2018 and is provided to the students
of this course only. Use by any other
individual without written consent of the author is forbidden.
These are more undamped SDOF problems for you to work on where the equivalent k or m must be obtained; or the frequency must be obtained using Rayleigh’s method or conservation of energy method.
Here are problems 2-17, 2-18, 2-19
Here are problems 2-26, 2-38
Here is the rest of 2-38, and problems 2-68, 2-79
Here is the rest of 2-79
Here is problem 2-69
Here is problem 2-33, problem 2-45, and problem 2-71
From here we begin Problems in free vibration with damping….
READ Chapter 2.6-2.8
Here is a videotape of materials on damped systems and log decrement.
Here is a videotape for coulomb friction
Here are problems 2.88 and 2.90
Here are problems 2.84, 2.92 and 2.95
Here are problems 2.93, 2.96 and the rest of 2.90
Here are problems 2.106, and 2.122
Here are problems 2.112, 2.113 and 2.115 part a
Here is the rest of 2.115 and 2.116 and the rest of 2.116
Here is problem 2.145
Some of these problem
solutions for the previous problem sets are not activated as they are under
copyright. Problems from the next set of
problems will be revealed when you have attempted them and you ask them to be
revealed.
Please do problems
2.17, 2.18, 2.19, 2.33, 2.88, 2.90, 2.106, 2.122 and they will be due on
9/28/18
First exam is announced for October 5 and will cover
materials from Chapters 1 and 2 of Rao’s book.
This
material and all the linked materials provided, except where stated
specifically, are copyrighted © Cesar Levy 2018 and is provided to the students
of this course only. Use by any other
individual without written consent of the author is forbidden.
Please start looking
at the following problems for systems with forcing functions
Here are problems 3.1, 3.2, 3.8, 3.10
Problems 3.19 and 3.25 are given in the back of your
book.
Here are problems 3.29 and 3.33part1, 3.33part2 and 3.32
Here is a videotape of forced vibration problems related to damped and undamped systems
On Lecture 11 we started discussing problems related to vibration of damped SDOF system with forcing functions, including beats, effects of adding damping to such sytems, resonance, how to find the magnification factor and where the maximum magnification factor is and how to calculate it.
Here
is a video related to beats,
undamped forced motion
On Lecture 12 we began discussing the topic of SDOF system with vibrating support and derived the equation of motion for it. The equation is similar to the forced vibration problem we began in Chapter 3 with Po =Y [k2 +(cwf)2]1/2 and the sine function now including a lag angle, b, i.e., sin (wf t - b).
On Lecture 13 we spoke of the
relative motion of a SDOF system with oscillating support and showed how this
case can be related to vibration measuring instruments such as vibrometers,
velometers and accelerometers. We did
problems 10.9 and 10.14 in Rao’s book.
Please read chapters 10-10.4.
Other problems of Chapter 3 to be
covered.
Here are problems 3.54, 3.58
Here are solutions to problem 3.53.
Problems 3.26, 3.48, 3.51 and 3.59 solutions can be viewed privately.
This
material and all the linked materials provided, except where stated specifically,
are copyrighted © Cesar Levy 2018 and is provided to the students of this
course only. Use by any other individual
without written consent of the author is forbidden.
These problems below
deal with force transmitted (chapter 9) and with vibration measuring equipment
(Chapter 10). Please go through them to
understand the concepts.
Here are problems 9.27, 9.32 and 9.34
Here is the rest of 9.34pt2 and 9.35
Here are problems 10.11, 10.12, 10.15
Here
is a video dealing with relative
motion and its importance in accelerometer design. Relative Motion is explained in Chapter 3,
but the applications are in Chapter 10.
A video dealing with problems
related to this topic as well as vibration absorber, accelerometers,
vibrometers can be found at the following link.
On Lecture 14 We had our first quiz
On Lecture 15 We spoke about the
power removed from a system due to a damper and showed that it varied like the
amplitude2. We the related
this to Q points (or half power points)
as a way in which to use experimental data to determine damping ratio, ζ,
in the case where the damping ratio is small.
We continued to speak about relative
motion and force transmitted to the oscillating support. We reviewed the case of a single degree of
freedom system with sinusoidal forcing function, namely
and showed that the Force
transmitted to the oscillating support base was = -m where x(t) was the
solution for the oscillating support.
This led to
= -mwf2 Xss,os
)
where Xss,os is the
steady state amplitude for the oscillating support. We did problem 9.27.
Lecture 16 you were asked to read
Chapter 9 on force transmitted and also asked to begin reading materials on the
rotating unbalance case.
Lecture 17 we spoke about the
rotating unbalance case as well as the force transmitted to the support due to
the rotating unbalance
This
material and all the linked materials provided, except where stated
specifically, are copyrighted © Cesar Levy 2018 and is provided to the students
of this course only. Use by any other
individual without written consent of the author is forbidden.
Here
is a video related to rotating
unbalance
Lecture 18 deals with solutions of
the SDOF systems with a general sinusoidal forcing function and also in the case
where the forcing function is NOT sinusoidal.
This begins Chapter 4 material.
Please start reading chapter 4 which deals with non-periodic forcing
functions of the type we discussed at the very end of the EML3222 classes (in
Chapter 9 of Rowell’s book).
You are assigned problems 4.15, 4.16
and 4.23. Once you have completed them,
you can view the solution below.
Lecture 19 and Lecture 20 will discuss displacements due to non-periodic forcing functions found in chapter 4. Once this material is covered, we will move on to two-degree of freedom systems found in Chapter 5 of Rao’s book.
Here are problems 4.15 and 4.16
Here is problem 4.23
Also for HW please do problem 4.12 and 4.13 (but let z=0.2
in this problem) using the methods we discussed
in class Due by 11/2
Exam
2 is announced for Nov 7.
The exam will cover forced vibration of a single degree of system (chapter 3) both damped and undamped, beats, force transmitted to support, oscillating support, rotating unbalance, relative motion, accelerometers, vibrometers (chapter 9 and 10 materials). Most of the materials that I talked about comes from Chapter 3, 9, 10. We also talked about other materials, namely, Q factor, and situations when the frequency ratio (r=wf/wn) is not due to changes in wf but changes in k and m.
You will be allowed 5 8.5 x 11 inch sheets of formulas. One of the 5 pages may be the page with the 4 graphs that I gave you, if you wish to use that.
This
material and all the linked materials provided, except where stated
specifically, are copyrighted © Cesar Levy 2018 and is provided to the students
of this course only. Use by any other
individual without written consent of the author is forbidden.
Lecture 21 and 22. 2 DOF systems
Chapter 5 begins two degree of freedom systems --linear motion, rotational systems, combined linear-rotational systems (like suspension type). Start reading Chapter 5, sections 1-5 and 7.
Here are problems that you should try: 5.1, 5.4, 5.5, 5.20, 5.21, 5.34. Only the first problem is worked out in its entirety for you to view. The others can be viewed privately.
Here
is a video dealing with problems for vibration
of 2DOF systems
Lecture
23 and 24. Application of 2DOF
equations. We start discussing the case
of the vibration absorber as an undamped method of reducing the amplitude of
vibration of the main mass.
Please
read chapter 9’s section on vibration absorber.
We had our second examination on Lesson
24.
Lectures
25 and 26 will cover the rest of 2-DOF problems and chapter 5, and, also will
include the 3rd exam.
We will have our third
examination on Nov 21 (change from what I
stated in class). The examination will
cover the materials in chapter 4 (SDOF under general forcing function-both
harmonic and non-harmonic), chapter 5 (2-DOF systems), Chapter 9 (vibration
absorbers).
Here
is a video dealing with problems for vibration
of 2DOF systems
Lesson
27 and 28 will start discussing the Rayleigh and Dunkerley methods of
determining natural frequencies. Chapter 7, Sections 1-3 begins solving 2 degree of
freedom systems numerically by using energy methods.
Problems for Chapter 7: Please do
Problems 5.1, 5.4, 5.55, 5.20, 5.21, 5.34 Using, Dunkerley and Using Rayleigh’s
methods and compare to the values you obtained (see problems above).
Practice on the problems 5.1, 5.4, 5.5, 5.20, 5.21, 5.34 by determining the
M and K matrices and using values for the vector A
This
material and all the linked materials provided, except where stated
specifically, are copyrighted © Cesar Levy 2018 and is provided to the students
of this course only. Use by any other
individual without written consent of the author is forbidden.
Please
read Chapter 5, Section 6 and its application found in Chapter 9, Sect 11. This will be the last topic to be discussed
in the course.
Please look at
problems 9.54, 9.57 and 9.60 that deal with this last topic. Please note that these problems will not be
uploaded but can be viewed privately if requested.
This
material and all the linked materials provided, except where stated
specifically, are copyrighted © Cesar Levy 2018 and is provided to the students
of this course only. Use by any other
individual without written consent of the author is forbidden.