Mechanical Engineering Projects

 

          The purpose of these projects is to relate linear algebra concepts to mechanical vibrations, especially resonance. While they use differential

equations, they do not assume any knowledge of differential equations on your part, only calculus 1 and 2.

 

 

Project #1  Forced vibrations      due Tuesday Nov 5  

 

          Your group should turn in a paper which covers mass-spring systems without damping but with an optional external force. After

            Newton’s Second Law is applied, this amounts to a differential equation of the form

 

                                    mx’’   +  kx  = f(t)

 

            where x stands for displacement from rest and t is time.  The external force is f(t), the mass m and the spring constant k.

            The    indicates a derivative with respect to time.

            (the word “show” is where work by you is required)

 

          Case #1:  homogeneous.   Assume no external force f(t)

 

                   Show that solutions to this  are   cos(w0t)   and  sin(w0t)      where  w0 = sqrt(k/m)  is called the “natural frequency”

 

                        Show that this problem is linear by showing that for any constant c  that

 

                                    1)     Ccos(w0t)   and  Csin(w0t)    are also solutions   

                                    2)      C1 cos(w0t)   +  C2 sin(w0t)      is also a solution

 

                        Question: in physics and mechanics, what is the Principle of Superposition?

 

          Case #2: nonhomogeneous.  External force f(t) present.

                   Note: this part requires only careful algebra and differential calculus.

 

                   Assume an external, oscillating force  f(t) = cos(wt)    and that w ¹ w0, above.

 

                        Show that a particular solution is  

 

                                                x(t) = cos(wt)/(m(w02 – w2))

 

                        Having done this, show that the general solution to the problem is

 

                                    x(t) =  C1 cos(w0t)   +  C2 sin(w0t)      + cos(wt)/(m(w02 – w2))   (c1  and c2 arbitrary)

 

                        Next, the solution must also satisfy initial conditions:

 

                                                x(0) = 0      (initially at the origin)

                                                            x’(0) = 0     (initially at rest – no velocity)

 

                             Pick  C1 and C2 so that these are satisfied 

         

                        What does your solution now look like?

 

                        Turn in a paper with a cover page listing all group members, the group number, and project number and title. The body may be a mix

of typing of text and hand printing of equations. List any resources (books, web, people).

 

Project #2:  The Mathematics of Resonance   Due Tuesday Nov 19

 

From Project #1, the solution to the initial value problem is

 

                                    x(t) =  (cos(wt)  -  cos(w0t) )/(m(w02 – w2))  

 

This is the basis for the second project.

 

First, consider the trig identities

 

                        cos(A+B) = cos(A)cos(B) –   sin(A)sin(B)

 

and                  cos(A-B) = cos(A)cos(B)  +  sin(A)sin(B)

 

Use them to write the solution from part 3 into one single term, instead of 2.  (hint: use the substitution  A = (w0 + w)/2  and  B = (w0 – w)/2 and do some algebra) I will be happy to tell you when you have it right!

 

5.  To make things interesting, lets try out some specific values for the frequencies. Take w0 = 2  and w = 2.1. What is significant here is that they are relatively close to one another (remember that w0 is the natural frequency and w the external or forcing frequency)

 

Graph the solution (easy in Maple with the plot function) and describe what you see in general terms. (suggestion t= 0 to 20 Pi or so to begin to get a sense of what’s going on).  The name for this phenomena is a beat.

 

 

6.      Resonance:  this happens when the natural and forcing frequencies match. We will find out what happens by considering w0 fixed and taking the limit as w -> w0.  Note that this results in an Indeterminate Form (remember those from Calc III??). Use LHopital’s Rule and  show that the solution becomes

 

t sin(w0t)/(2mw0)

 

      (the t in front is significant!)

 

7.      Graph the resonant solution and describe what you see

 

 

 

                        Project #3:  Examples involving Resonance   due Tuesday Dec 3

 

The basis for this project is two video tapes (available in the library on reserve ) as well as a talk on resonance

by Professor Dimentberg of the Mechanical Engineering Department.  Your paper should

 

a)      summarize his talk

 

b)      explain how resonance takes place in both of the physical situations videotaped