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Math 431 Solution of Midterm 2 Fall 1999

  1. (18 points) Find the general solution of the following equation:

    displaymath289

    Answer: The characteristic equation tex2html_wrap_inline331 has roots tex2html_wrap_inline333 and tex2html_wrap_inline335 . Hence, the general solution has the form

    displaymath290

    where tex2html_wrap_inline337 and tex2html_wrap_inline339 are particular solutions of the non-homogenous equations L[y]=2t+1 and tex2html_wrap_inline343 . We find these particular solutions of the form tex2html_wrap_inline345 and tex2html_wrap_inline347 using the method of undetermined coefficients. Plugging tex2html_wrap_inline337 into the equation we get the equation

    eqnarray22

    We conclude that tex2html_wrap_inline351 .

    Plugging tex2html_wrap_inline347 into the equation we get

    displaymath291

    Hence, tex2html_wrap_inline355 . The general solution is

    displaymath292

  2. (16 points) Solve the following initial value problem

    displaymath293

    Answer: (Compare with homework problem 5 in Section 3.7) The roots of the characteristic equation tex2html_wrap_inline357 are tex2html_wrap_inline359 . Hence, tex2html_wrap_inline361 and tex2html_wrap_inline363 are a fundamental pair of solutions. Their Wronskian is

    displaymath294

    The method of variation of parameters helps us find the solution to the initial value problem via the formula (using definite integration)

    eqnarray49

    Another (longer) method would be to use indefinite integration in the formula of variation of parameters to find a particular solution Y(t). One then determines the constants tex2html_wrap_inline367 and tex2html_wrap_inline369 for which tex2html_wrap_inline371 satisfies y(0)=0 and y'(0)=0.

  3. (16 points) Find the general solution of the equation tex2html_wrap_inline377 You may use the fact that tex2html_wrap_inline379 is a solution.

    Answer: First method: Most students found the general solution using the method of reduction of order. We are given that tex2html_wrap_inline381 is a solution. We look for a second solution of the form tex2html_wrap_inline383 where v(t) satisfies the differential equation

    displaymath295

    Above, tex2html_wrap_inline387 is the coefficient of y' in the normalized equation. Integrating both sides, we get

    eqnarray82

    Hence, tex2html_wrap_inline391 .

    Second Method: An easy way to find the general solution would be to realize that the equation is an Euler equation (see homework problems 38 and 39 in Section 3.4). We solve it by looking for a solution of the form tex2html_wrap_inline393 . Plugging into the equation we get

    displaymath296

    The two solutions of the equation tex2html_wrap_inline395 are tex2html_wrap_inline397 and tex2html_wrap_inline399 . Hence, the general solution is tex2html_wrap_inline401

  4. (20 points) The position function of an undampped spring mass system is determined by the initial value problem

      equation97

    a) (10 points) Find the solution of the system if the frequency tex2html_wrap_inline403 of the external force is 1.

    Answer: The solutions of the characteristic equation tex2html_wrap_inline407 are tex2html_wrap_inline409 and tex2html_wrap_inline411 . The general solution has the form

    displaymath297

    and a particular solution tex2html_wrap_inline413 can be found using the method of undetermined coefficient. Plugging tex2html_wrap_inline415 into the equation we get

    displaymath298

    and equating coefficients, we get tex2html_wrap_inline417 and B=0 and the general solution is

    displaymath299

    The initial condition determines that tex2html_wrap_inline421 and tex2html_wrap_inline423 . The solution is thus

    displaymath300

    b) (3 points) What is the frequency tex2html_wrap_inline403 of the external force which will cause the system to resonate (oscillate with increasing amplitude)? Justify your answer!!!

    Answer: The method of undetermined coefficients tells us that the equation (1) has a particular solution of the form

    displaymath301

    with s=0 if tex2html_wrap_inline429 and s=1 if tex2html_wrap_inline433 . Hence, resonance occurs when s=1, i.e., when the frequency tex2html_wrap_inline403 of the external force is equal to the frequency 8 of the homogeneous equation.

    c) (4 points) Find the solution of the resonating system when the frequency tex2html_wrap_inline403 is the one from part b.

    Answer: The equation tex2html_wrap_inline443 has a particular solution of the form

    displaymath302

    Differentiating twice, we get tex2html_wrap_inline445 Plugging Y(t) into the equation, we get

    eqnarray121

    Thus tex2html_wrap_inline449 and A=0 and

    displaymath303

    One checks that it satisfies the initial condition.

    d) (3 points) Carefully graph the solution of the resonating system in part c in the time interval tex2html_wrap_inline453 . Indicate all the t-axis intercepts.

  5. (20 points) A damped spring mass system is governed by the equation

    displaymath304

    where tex2html_wrap_inline457 is a positive constant which depends on the damper.

    a) (8 points) Solve the system if tex2html_wrap_inline459 and tex2html_wrap_inline461 , u'(0)=0.

    Answer: The two roots of the characteristic equation tex2html_wrap_inline465 are

    displaymath305

    The general solution is tex2html_wrap_inline467 The initial condition determines tex2html_wrap_inline469 , tex2html_wrap_inline471 , and

      equation143

    b) (6 points) Graph your solution in part a. Determine the quasi-period and all points of time at which the mass passes through the equilibrium.

    Answer: We first rewrite the solution (2) in the form

    eqnarray156

    The quasi-period is tex2html_wrap_inline473 . The mass returns to its equilibrium when u(t)=0, i.e., when

    displaymath306

    Solving for t we get

    eqnarray182

    c) (6 points) Determine the range of values of tex2html_wrap_inline457 for which the position function u(t) is a decaying oscillation? Justify your answer!!!

    Answer: The position function u(t) is a decaying oscilation precisely when the roots of the characteristic equation are complex with a strictly negative real part. If the roots

    displaymath307

    are such, then the solution tex2html_wrap_inline485 is decaying (because tex2html_wrap_inline487 ) and oscilating (because tex2html_wrap_inline489 ). This happens precisely when tex2html_wrap_inline491 and tex2html_wrap_inline493 , i.e., when

    displaymath308

  6. (10 points) A mass weighing tex2html_wrap_inline495 stretches a spring tex2html_wrap_inline497 . The mass is acted upon by an external force of tex2html_wrap_inline499 . The mass is also attached to a damper with damping constant . Set up an initial value problem for the position u(t) of the mass t seconds after it was pulled down (in the positive direction) tex2html_wrap_inline507 and set in motion downwards with an initial velocity of tex2html_wrap_inline509 . (Recall that the gravitational constant g is ). Do NOT solve the initial value problem!

    Answer: The spring mass system satisfies the differential equation:

    displaymath309

    The information given translates to

    eqnarray218

    We get that the mass is tex2html_wrap_inline515 and the spring constant is tex2html_wrap_inline517 . The initial value problem is thus

    eqnarray238




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Eyal Markman
Fri Nov 26 10:14:09 EST 1999