Math 431 Solution of Midterm 2 Fall 1999
Answer: The characteristic equation has roots and . Hence, the general solution has the form
where and are particular solutions of the non-homogenous equations L[y]=2t+1 and . We find these particular solutions of the form and using the method of undetermined coefficients. Plugging into the equation we get the equation
We conclude that .
Plugging into the equation we get
Hence, . The general solution is
Answer: (Compare with homework problem 5 in Section 3.7) The roots of the characteristic equation are . Hence, and are a fundamental pair of solutions. Their Wronskian is
The method of variation of parameters helps us find the solution to the initial value problem via the formula (using definite integration)
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 and for which satisfies y(0)=0 and y'(0)=0.
Answer: First method: Most students found the general solution using the method of reduction of order. We are given that is a solution. We look for a second solution of the form where v(t) satisfies the differential equation
Above, is the coefficient of y' in the normalized equation. Integrating both sides, we get
Hence, .
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 . Plugging into the equation we get
The two solutions of the equation are and . Hence, the general solution is
a) (10 points) Find the solution of the system if the frequency of the external force is 1.
Answer: The solutions of the characteristic equation are and . The general solution has the form
and a particular solution can be found using the method of undetermined coefficient. Plugging into the equation we get
and equating coefficients, we get and B=0 and the general solution is
The initial condition determines that and . The solution is thus
b) (3 points) What is the frequency 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
with s=0 if and s=1 if . Hence, resonance occurs when s=1, i.e., when the frequency 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 is the one from part b.
Answer: The equation has a particular solution of the form
Differentiating twice, we get Plugging Y(t) into the equation, we get
Thus and A=0 and
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 . Indicate all the t-axis intercepts.
where is a positive constant which depends on the damper.
a) (8 points) Solve the system if and , u'(0)=0.
Answer: The two roots of the characteristic equation are
The general solution is The initial condition determines , , and
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
The quasi-period is . The mass returns to its equilibrium when u(t)=0, i.e., when
Solving for t we get
c) (6 points) Determine the range of values of 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
are such, then the solution is decaying (because ) and oscilating (because ). This happens precisely when and , i.e., when
Answer: The spring mass system satisfies the differential equation:
The information given translates to
We get that the mass is and the spring constant is . The initial value problem is thus