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Mathematics LibreTexts

17.R: Chapter 17 Review Exercises

  • Gilbert Strang & Edwin “Jed” Herman
  • OpenStax

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True or False? Justify your answer with a proof or a counterexample.

1. If y and z are both solutions to y+2y+y=0, then y+z is also a solution.

Answer
True

2. The following system of algebraic equations has a unique solution:

6z1+3z2=84z1+2z2=4.

3. y=excos(3x)+exsin(2x) is a solution to the second-order differential equation y+2y+10=0.

Answer
False

4. To find the particular solution to a second-order differential equation, you need one initial condition.

In problems 5 - 8, classify the differential equations. Determine the order, whether it is linear and, if linear, whether the differential equation is homogeneous or nonhomogeneous. If the equation is second-order homogeneous and linear, find the characteristic equation.

5. y2y=0

Answer
second order, linear, homogeneous, λ22=0

6. y3y+2y=cos(t)

7. (dydt)2+yy=1

Answer
first order, nonlinear, nonhomogeneous

8. d2ydt2+tdydt+sin2(t)y=et

In problems 9 - 16, find the general solution.

9. y+9y=0

Answer
y=c1sin(3x)+c2cos(3x)

10. y+2y+y=0

11. y2y+10y=4x

Answer
y=c1exsin(3x)+c2excos(3x)+25x+225

12. y=cos(x)+2y+y

13. y+5y+y=x+e2x

Answer
y=c1ex+c2e4x+x4+e2x18516

14. y=3y+xex

15. yx2=3y94y+3x

Answer
y=c1e(3/2)x+c2xe(3/2)x+49x2+427x1627

16. y=2cosx+yy

In problems 17 - 18, find the solution to the initial-value problem, if possible.

17. y+4y+6y=0,y(0)=0,y(0)=2

Answer
y=e2xsin(2x)

18. y=3ycos(x),y(0)=94,y(0)=0

In problems 19 - 20, find the solution to the boundary-value problem.

19. 4y=6y+2y,y(0)=0,y(1)=1

Answer
y=e1xe41(e4x1)

20. y=3xyy,y(0)=3,y(1)=0

For the following problem, set up and solve the differential equation.

21. The motion of a swinging pendulum for small angles θ can be approximated by d2θdt2+gLθ=0, where θ is the angle the pendulum makes with respect to a vertical line, g is the acceleration resulting from gravity, and L is the length of the pendulum. Find the equation describing the angle of the pendulum at time t, assuming an initial displacement of θ0 and an initial velocity of zero.

Answer
θ(t)=θ0cos(glt)

In problems 22 - 23, consider the “beats” that occur when the forcing term of a differential equation causes “slow” and “fast” amplitudes. Consider the general differential equation ay+by=cos(ωt) that governs undamped motion. Assume that baω.

22. Find the general solution to this equation (Hint: call ω0=b/a).

23. Assuming the system starts from rest, show that the particular solution can be written asy=2a(ω20ω2)sin(ω0ωt2)sin(ω0+ωt2).

24. [T] Using your solutions derived earlier, plot the solution to the system 2y+9y=cos(2t) over the interval t=[50,50]. Find, analytically, the period of the fast and slow amplitudes.

For the following problem, set up and solve the differential equations.

25. An opera singer is attempting to shatter a glass by singing a particular note. The vibrations of the glass can be modeled by y+ay=cos(bt), where y+ay=0 represents the natural frequency of the glass and the singer is forcing the vibrations at cos(bt). For what value b would the singer be able to break that glass? (Note: in order for the glass to break, the oscillations would need to get higher and higher.)

Answer
b=a

This page titled 17.R: Chapter 17 Review Exercises is shared under a CC BY-NC-SA 4.0 license and was authored, remixed, and/or curated by Gilbert Strang & Edwin “Jed” Herman (OpenStax) via source content that was edited to the style and standards of the LibreTexts platform.

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