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CHAPTER 1 Review Problems
The main objective of this set of review problems is practice in the identification of the different
types of first-order differential equations discussed in this chapter. In each of Problems 1-36 we
identify the type of the given equation and indicate an appropriate method of solution.

1.     If we write the equation in the form y′ − (3 / x ) y = x 2 we see that it is linear with
       integrating factor ρ = x −3 . The method of Section 1.5 then yields the general solution
       y = x3(C + ln x).

2.     We write this equation in the separable form y′ / y 2 = ( x + 3) / x 2 . Then separation of
       variables and integration as in Section 1.4 yields the general solution
       y = x / (3 – Cx – x ln x).

3.     This equation is homogeneous. The substitution y = vx of Equation (8) in Section 1.6
       leads to the general solution y = x/(C – ln x).

4.                       (
       We note that Dy 2 xy 3 + e x   )=      (              )
                                           Dx 3 x 2 y 2 + sin y = 6 xy 2 , so the given equation is
       exact. The method of Example 9 in Section 1.6 yields the implicit general solution
       x2y3 + ex – cos y = C.

5.     We write this equation in the separable form y′ / y 2 = (2 x − 3) / x 4 . Then separation
       of variables and integration as in Section 1.4 yields the general solution
       y = C exp[(1 – x)/x3].

6.     We write this equation in the separable form y′ / y 2 = (1 − 2 x) / x 2 . Then separation
       of variables and integration as in Section 1.4 yields the general solution
       y = x / (1 + Cx + 2x ln x).

7.     If we write the equation in the form y′ + (2 / x) y = 1/ x 3 we see that it is linear with
       integrating factor ρ = x 2 . The method of Section 1.5 then yields the general solution
       y = x–2(C + ln x).

8.     This equation is homogeneous. The substitution y = vx of Equation (8) in Section 1.6
       leads to the general solution y = 3Cx/(C – x3).

9.     If we write the equation in the form y′ + (2 / x) y = 6 x y we see that it is a Bernoulli
       equation with n = 1/2. The substitution v = y −1/ 2 of Eq. (10) in Section 1.6 then
       yields the general solution y = (x2 + C/x)2.

10.                                                          (       )
       We write this equation in the separable form y′ / 1 + y 2 = 1 + x 2 . Then separation
       of variables and integration as in Section 1.4 yields the general solution


Chapter 1 Review                                                                               1
y = tan(C + x + x3/3).

11.   This equation is homogeneous. The substitution y = vx of Equation (8) in Section 1.6
      leads to the general solution y = x / (C – 3 ln x).

12.                      (            )           (                )
      We note that Dy 6 xy 3 + 2 y 4 = Dx 9 x 2 y 2 + 8 xy 3 = 18 xy 2 + 8 y 3 , so the given
      equation is exact. The method of Example 9 in Section 1.6 yields the implicit general
      solution 3x2y3 + 2xy4 = C.

13.   We write this equation in the separable form y′ / y 2 = 5 x 4 − 4 x. Then separation
      of variables and integration as in Section 1.4 yields the general solution
      y = 1 / (C + 2x2 – x5).

14.   This equation is homogeneous. The substitution y = vx of Equation (8) in Section 1.6
      leads to the implicit general solution y2 = x2 / (C + 2 ln x).

15.   This is a linear differential equation with integrating factor ρ = e3 x . The method of
      Section 1.5 yields the general solution y = (x3 + C)e-3x.

16.   The substitution v = y − x, y = v + x, y′ = v′ + 1 gives the separable equation
      v′ + 1 = ( y − x) 2 = v 2 in the new dependent variable v. The resulting implicit general
      solution of the original equation is y – x – 1 = C e2x(y – x + 1).

17.                      (
      We note that Dy e x + y e x y   )=      (
                                           Dx e y + x e x y   )=   e x y + xy e x y , so the given equation is
      exact. The method of Example 9 in Section 1.6 yields the implicit general solution
      ex + ey + ex y = C.

18.   This equation is homogeneous. The substitution y = vx of Equation (8) in Section 1.6
      leads to the implicit general solution y2 = Cx2(x2 – y2).

19.                                                                      (        )
      We write this equation in the separable form y′ / y 2 = 2 − 3x 5 / x 3 . Then separation
      of variables and integration as in Section 1.4 yields the general solution
      y = x2 / (x5 + Cx2 + 1).

20.   If we write the equation in the form y′ + (3 / x) y = 3 x −5 / 2 we see that it is linear with
      integrating factor ρ = x 3 . The method of Section 1.5 then yields the general solution
      y = 2x–3/2 + Cx–3.

21.   If we write the equation in the form y′ + (1/( x + 1) ) y = 1/( x 2 − 1) we see that it is linear
      with integrating factor ρ = x + 1. The method of Section then 1.5 yields the general
      solution y = [C + ln(x – 1)] / (x + 1).



Chapter 1 Review                                                                                     2
22.   If we write the equation in the form y′ − (6 / x) y = 12 x 3 y 2 / 3 we see that it is a Bernoulli
      equation with n = 1/3. The substitution v = y −2 / 3 of Eq. (10) in Section 1.6 then
      yields the general solution y = (2x4 + Cx2)3.

23.                         (              )         (                  )
      We note that Dy e y + y cos x = Dx x e y + sin x = e y + cos x, so the given equation
      is exact. The method of Example 9 in Section 1.6 yields the implicit general solution
      x ey + y sin x = C

24.                                                                         (         )
      We write this equation in the separable form y′ / y 2 = 1 − 9 x 2 / x 3/ 2 . Then separation
      of variables and integration as in Section 1.4 yields the general solution
      y = x1/2 / (6x2 + Cx1/2 + 2).

25.   If we write the equation in the form y′ + ( 2 /( x + 1) ) y = 3 we see that it is linear with
      integrating factor ρ = ( x + 1) . The method of Section 1.5 then yields the general
                                           2


      solution y = x + 1 + C (x + 1)–2.

26.                         (                            )          (                      )
      We note that Dy 9 x1/ 2 y 4 / 3 − 12 x1/ 5 y 3/ 2 = Dx 8 x 3/ 2 y1/ 3 − 15 x 6 / 5 y1/ 2 =
      12 x1/ 2 y1/ 3 − 18 x1/ 5 y1/ 2 , so the given equation is exact. The method of Example 9 in
      Section 1.6 yields the implicit general solution 6x3/2y4/3 – 10x6/5y3/2 = C.

27.   If we write the equation in the form y′ + (1/ x) y = − x 2 y 4 / 3 we see that it is a Bernoulli
      equation with n = 4. The substitution v = y −3 of Eq. (10) in Section 1.6 then yields
      the general solution y = x–1(C + ln x)–1/3.

28.   If we write the equation in the form y′ + (1/ x) y = 2 e 2 x / x we see that it is linear with
      integrating factor ρ = x. The method of Section 1.5 then yields the general solution
      y = x–1(C + e2x).

29.   If we write the equation in the form y′ + (1/(2 x + 1) ) y = (2 x + 1)1/ 2 we see that it is
      linear with integrating factor ρ = ( 2 x + 1) . The method of Section 1.5 then yields
                                                             1/ 2


      the general solution y = (x2 + x + C)(2x + 1)–1/2.

30.   The substitution v = x + y, y = v − x, y′ = v′ − 1 gives the separable equation
       v′ − 1 = v in the new dependent variable v. The resulting implicit general solution of
      the original equation is x = 2(x + y)1/2 – 2 ln[1 + (x + y)1/2] + C.

31.   dy /( y + 7) = 3x 2 is separable; y′ + 3x 2 y = 21x 2 is linear.

32.   dy /( y 2 − 1) = x is separable; y′ + x y = x y 3 is a Bernoulli equation with n = 3.



Chapter 1 Review                                                                                   3
33.   (3x 2 + 2 y 2 ) dx + 4 xy dy = 0 is exact; y′ = − 1 (3x / y + 2 y / x ) is homogeneous.
                                                        4



                                                         1+ 3y / x
34.   ( x + 3 y ) dx + (3x − y ) dy = 0 is exact; y′ =             is homogeneous.
                                                          y / x−3

35.                        (      )                      (           )
      dy /( y + 1) = 2 x / x 2 + 1 is separable; y′ − 2 x /( x 2 + 1) y = 2 x /( x 2 + 1) is linear.


36.   dy /   (        )
                 y − y = cot x is separable; y′ + (cot x ) y = (cot x) y is a Bernoulli equation
      with n = 1/2.




Chapter 1 Review                                                                                 4

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Sect1 R

  • 1. CHAPTER 1 Review Problems The main objective of this set of review problems is practice in the identification of the different types of first-order differential equations discussed in this chapter. In each of Problems 1-36 we identify the type of the given equation and indicate an appropriate method of solution. 1. If we write the equation in the form y′ − (3 / x ) y = x 2 we see that it is linear with integrating factor ρ = x −3 . The method of Section 1.5 then yields the general solution y = x3(C + ln x). 2. We write this equation in the separable form y′ / y 2 = ( x + 3) / x 2 . Then separation of variables and integration as in Section 1.4 yields the general solution y = x / (3 – Cx – x ln x). 3. This equation is homogeneous. The substitution y = vx of Equation (8) in Section 1.6 leads to the general solution y = x/(C – ln x). 4. ( We note that Dy 2 xy 3 + e x )= ( ) Dx 3 x 2 y 2 + sin y = 6 xy 2 , so the given equation is exact. The method of Example 9 in Section 1.6 yields the implicit general solution x2y3 + ex – cos y = C. 5. We write this equation in the separable form y′ / y 2 = (2 x − 3) / x 4 . Then separation of variables and integration as in Section 1.4 yields the general solution y = C exp[(1 – x)/x3]. 6. We write this equation in the separable form y′ / y 2 = (1 − 2 x) / x 2 . Then separation of variables and integration as in Section 1.4 yields the general solution y = x / (1 + Cx + 2x ln x). 7. If we write the equation in the form y′ + (2 / x) y = 1/ x 3 we see that it is linear with integrating factor ρ = x 2 . The method of Section 1.5 then yields the general solution y = x–2(C + ln x). 8. This equation is homogeneous. The substitution y = vx of Equation (8) in Section 1.6 leads to the general solution y = 3Cx/(C – x3). 9. If we write the equation in the form y′ + (2 / x) y = 6 x y we see that it is a Bernoulli equation with n = 1/2. The substitution v = y −1/ 2 of Eq. (10) in Section 1.6 then yields the general solution y = (x2 + C/x)2. 10. ( ) We write this equation in the separable form y′ / 1 + y 2 = 1 + x 2 . Then separation of variables and integration as in Section 1.4 yields the general solution Chapter 1 Review 1
  • 2. y = tan(C + x + x3/3). 11. This equation is homogeneous. The substitution y = vx of Equation (8) in Section 1.6 leads to the general solution y = x / (C – 3 ln x). 12. ( ) ( ) We note that Dy 6 xy 3 + 2 y 4 = Dx 9 x 2 y 2 + 8 xy 3 = 18 xy 2 + 8 y 3 , so the given equation is exact. The method of Example 9 in Section 1.6 yields the implicit general solution 3x2y3 + 2xy4 = C. 13. We write this equation in the separable form y′ / y 2 = 5 x 4 − 4 x. Then separation of variables and integration as in Section 1.4 yields the general solution y = 1 / (C + 2x2 – x5). 14. This equation is homogeneous. The substitution y = vx of Equation (8) in Section 1.6 leads to the implicit general solution y2 = x2 / (C + 2 ln x). 15. This is a linear differential equation with integrating factor ρ = e3 x . The method of Section 1.5 yields the general solution y = (x3 + C)e-3x. 16. The substitution v = y − x, y = v + x, y′ = v′ + 1 gives the separable equation v′ + 1 = ( y − x) 2 = v 2 in the new dependent variable v. The resulting implicit general solution of the original equation is y – x – 1 = C e2x(y – x + 1). 17. ( We note that Dy e x + y e x y )= ( Dx e y + x e x y )= e x y + xy e x y , so the given equation is exact. The method of Example 9 in Section 1.6 yields the implicit general solution ex + ey + ex y = C. 18. This equation is homogeneous. The substitution y = vx of Equation (8) in Section 1.6 leads to the implicit general solution y2 = Cx2(x2 – y2). 19. ( ) We write this equation in the separable form y′ / y 2 = 2 − 3x 5 / x 3 . Then separation of variables and integration as in Section 1.4 yields the general solution y = x2 / (x5 + Cx2 + 1). 20. If we write the equation in the form y′ + (3 / x) y = 3 x −5 / 2 we see that it is linear with integrating factor ρ = x 3 . The method of Section 1.5 then yields the general solution y = 2x–3/2 + Cx–3. 21. If we write the equation in the form y′ + (1/( x + 1) ) y = 1/( x 2 − 1) we see that it is linear with integrating factor ρ = x + 1. The method of Section then 1.5 yields the general solution y = [C + ln(x – 1)] / (x + 1). Chapter 1 Review 2
  • 3. 22. If we write the equation in the form y′ − (6 / x) y = 12 x 3 y 2 / 3 we see that it is a Bernoulli equation with n = 1/3. The substitution v = y −2 / 3 of Eq. (10) in Section 1.6 then yields the general solution y = (2x4 + Cx2)3. 23. ( ) ( ) We note that Dy e y + y cos x = Dx x e y + sin x = e y + cos x, so the given equation is exact. The method of Example 9 in Section 1.6 yields the implicit general solution x ey + y sin x = C 24. ( ) We write this equation in the separable form y′ / y 2 = 1 − 9 x 2 / x 3/ 2 . Then separation of variables and integration as in Section 1.4 yields the general solution y = x1/2 / (6x2 + Cx1/2 + 2). 25. If we write the equation in the form y′ + ( 2 /( x + 1) ) y = 3 we see that it is linear with integrating factor ρ = ( x + 1) . The method of Section 1.5 then yields the general 2 solution y = x + 1 + C (x + 1)–2. 26. ( ) ( ) We note that Dy 9 x1/ 2 y 4 / 3 − 12 x1/ 5 y 3/ 2 = Dx 8 x 3/ 2 y1/ 3 − 15 x 6 / 5 y1/ 2 = 12 x1/ 2 y1/ 3 − 18 x1/ 5 y1/ 2 , so the given equation is exact. The method of Example 9 in Section 1.6 yields the implicit general solution 6x3/2y4/3 – 10x6/5y3/2 = C. 27. If we write the equation in the form y′ + (1/ x) y = − x 2 y 4 / 3 we see that it is a Bernoulli equation with n = 4. The substitution v = y −3 of Eq. (10) in Section 1.6 then yields the general solution y = x–1(C + ln x)–1/3. 28. If we write the equation in the form y′ + (1/ x) y = 2 e 2 x / x we see that it is linear with integrating factor ρ = x. The method of Section 1.5 then yields the general solution y = x–1(C + e2x). 29. If we write the equation in the form y′ + (1/(2 x + 1) ) y = (2 x + 1)1/ 2 we see that it is linear with integrating factor ρ = ( 2 x + 1) . The method of Section 1.5 then yields 1/ 2 the general solution y = (x2 + x + C)(2x + 1)–1/2. 30. The substitution v = x + y, y = v − x, y′ = v′ − 1 gives the separable equation v′ − 1 = v in the new dependent variable v. The resulting implicit general solution of the original equation is x = 2(x + y)1/2 – 2 ln[1 + (x + y)1/2] + C. 31. dy /( y + 7) = 3x 2 is separable; y′ + 3x 2 y = 21x 2 is linear. 32. dy /( y 2 − 1) = x is separable; y′ + x y = x y 3 is a Bernoulli equation with n = 3. Chapter 1 Review 3
  • 4. 33. (3x 2 + 2 y 2 ) dx + 4 xy dy = 0 is exact; y′ = − 1 (3x / y + 2 y / x ) is homogeneous. 4 1+ 3y / x 34. ( x + 3 y ) dx + (3x − y ) dy = 0 is exact; y′ = is homogeneous. y / x−3 35. ( ) ( ) dy /( y + 1) = 2 x / x 2 + 1 is separable; y′ − 2 x /( x 2 + 1) y = 2 x /( x 2 + 1) is linear. 36. dy / ( ) y − y = cot x is separable; y′ + (cot x ) y = (cot x) y is a Bernoulli equation with n = 1/2. Chapter 1 Review 4