Concordia University                                                            February 9, 2010

                       Applied Ordinary Differential Equations
                               ENGR 213 - Section F
                                  Prof. Alina Stancu

                                           Exam I (B)



   (1) (10 points) Solve the initial value problem

                                     dy
                              (x2 + 4)  + 2xy = x, y(0) = 1.
                                     dx
         Solution: An integrating factor is
                                          2x
                                                 dx         2 +4)
                            µ(x) = e     x2 +4        = eln(x       = x2 + 4.
         Multiplying both sides of the ODE with this integrating factor leads to
                                         (x2 + 4) y         = x.
         Integrating both sides with respect to x, we obtain
                                x2               x2 /2 + C
                   (x2 + 4) y =    +C ⇒ y =                , C = constant.
                                2                 x2 + 4
        We use y(0) = 1 to find the constant C as y(0) = C/4 = 1 ⇒ C = 4, thus the
      solution to the IVP is
                                x2 /2 + 4            x2 + 8
                          y(x) = 2        or y(x) = 2       .
                                 x +4               2x + 8

   (2) (10 points) Solve the given homogeneous equation by the appropriate substitution

                                         dy   3x2 + 2y 2
                                            =            .
                                         dx      4xy

      You may leave the solution in implicit form.
        Solution: We use the standard substitution for homogeneous ODEs of first order,
                                          dy
      namely u = y/x or y = ux and, thus, dx = x du + u.
                                                 dx
         Therefore the ODE becomes
                          du       3 + 2u2     du   3 − 2u2
                        x    +u=           ⇒ x    =         .
                          dx         4u        dx     4u
                                         4u       1
         The latter is a separable ODE 3−2u2 du = x dx. Integrating, we obtain − ln |3−2u2 | =
      ln |x| + C, where C is an arbitrary constant.
         Hence we obtain the solution y(x), in implicit form, of the original ODE
                                                       1
2



                        − ln |3 − 2(y/x)2 | = ln |x| + C, C = constant.

    (3) (10 points) Solve the exact ordinary differential equation

                        √               x                     y
                            x+                     dx +                     dy = 0,
                                    x2 + y 2 + 1          x2 + y 2 + 1

          leaving the solution in implicit form.
          Solution: We seek a function φ(x, y) such that
                     ∂φ √               x         ∂φ                    y
                        = x+                    ,     =                           .
                     ∂x            x 2 + y2 + 1   ∂y              x2   + y2 + 1
          Integrating the first equation with respect to x, we obtain
          φ(x, y) = 2 x3/2 + x2 + y 2 + 1 + c(y). Consequently,
                    3
           ∂φ           y
              =                    + c (y) ⇒ c (y) = 0 ⇒ c(y) = C, C = constant.
           ∂y       x2 + y 2 + 1
          It follows that the solution to the exact ODE (given in implicit form) is
                           2 3/2                     ˜ ˜
                             x + x2 + y 2 + 1 = C, C = constant.
                           3

    (4) (10 points) A pitcher of buttermilk initially at 25◦ C is to be cooled by setting it on
        the front porch, where the temperature is 5◦ C. Suppose that the temperature of the
        buttermilk has dropped to 15◦ C after 20 minutes. When will it be at 10◦ C?
         Solution: Newton’s model of cooling tells us that the ODE describing the tempera-
       ture of the cake T (t) is
        dT
           = −K(T − 5), T (0) = 25, T (20) = 15, K = a constant to be determined.
        dt
          We solve first for the general solution of the ODE (which we treat as separable):
                  1
                      dT = −K dt ⇒ ln |T − 5| = −Kt + C, C = constant.
               T −5
         Using T (0) = 25 and T (20) = 15, we obtain C = ln 20 and ln 10 = −20K + ln 20 ⇒
       20K = ln 2 ⇒ K = (ln 2)/20.
          Thus
                                                                                  t/20
                                                                              1
                    T = 5 + e−Kt+C = 5 + e−t(ln 2)/20+ln 20 = 5 + 20
                                                                              2
          and

                            t/20
                        1
          10 = 5 + 20              ⇒ t = 20 ln(5/20)/ ln(1/2) = 20 ln(4)/ ln 2 = 40 min.
                        2

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  • 1. Concordia University February 9, 2010 Applied Ordinary Differential Equations ENGR 213 - Section F Prof. Alina Stancu Exam I (B) (1) (10 points) Solve the initial value problem dy (x2 + 4) + 2xy = x, y(0) = 1. dx Solution: An integrating factor is 2x dx 2 +4) µ(x) = e x2 +4 = eln(x = x2 + 4. Multiplying both sides of the ODE with this integrating factor leads to (x2 + 4) y = x. Integrating both sides with respect to x, we obtain x2 x2 /2 + C (x2 + 4) y = +C ⇒ y = , C = constant. 2 x2 + 4 We use y(0) = 1 to find the constant C as y(0) = C/4 = 1 ⇒ C = 4, thus the solution to the IVP is x2 /2 + 4 x2 + 8 y(x) = 2 or y(x) = 2 . x +4 2x + 8 (2) (10 points) Solve the given homogeneous equation by the appropriate substitution dy 3x2 + 2y 2 = . dx 4xy You may leave the solution in implicit form. Solution: We use the standard substitution for homogeneous ODEs of first order, dy namely u = y/x or y = ux and, thus, dx = x du + u. dx Therefore the ODE becomes du 3 + 2u2 du 3 − 2u2 x +u= ⇒ x = . dx 4u dx 4u 4u 1 The latter is a separable ODE 3−2u2 du = x dx. Integrating, we obtain − ln |3−2u2 | = ln |x| + C, where C is an arbitrary constant. Hence we obtain the solution y(x), in implicit form, of the original ODE 1
  • 2. 2 − ln |3 − 2(y/x)2 | = ln |x| + C, C = constant. (3) (10 points) Solve the exact ordinary differential equation √ x y x+ dx + dy = 0, x2 + y 2 + 1 x2 + y 2 + 1 leaving the solution in implicit form. Solution: We seek a function φ(x, y) such that ∂φ √ x ∂φ y = x+ , = . ∂x x 2 + y2 + 1 ∂y x2 + y2 + 1 Integrating the first equation with respect to x, we obtain φ(x, y) = 2 x3/2 + x2 + y 2 + 1 + c(y). Consequently, 3 ∂φ y = + c (y) ⇒ c (y) = 0 ⇒ c(y) = C, C = constant. ∂y x2 + y 2 + 1 It follows that the solution to the exact ODE (given in implicit form) is 2 3/2 ˜ ˜ x + x2 + y 2 + 1 = C, C = constant. 3 (4) (10 points) A pitcher of buttermilk initially at 25◦ C is to be cooled by setting it on the front porch, where the temperature is 5◦ C. Suppose that the temperature of the buttermilk has dropped to 15◦ C after 20 minutes. When will it be at 10◦ C? Solution: Newton’s model of cooling tells us that the ODE describing the tempera- ture of the cake T (t) is dT = −K(T − 5), T (0) = 25, T (20) = 15, K = a constant to be determined. dt We solve first for the general solution of the ODE (which we treat as separable): 1 dT = −K dt ⇒ ln |T − 5| = −Kt + C, C = constant. T −5 Using T (0) = 25 and T (20) = 15, we obtain C = ln 20 and ln 10 = −20K + ln 20 ⇒ 20K = ln 2 ⇒ K = (ln 2)/20. Thus t/20 1 T = 5 + e−Kt+C = 5 + e−t(ln 2)/20+ln 20 = 5 + 20 2 and t/20 1 10 = 5 + 20 ⇒ t = 20 ln(5/20)/ ln(1/2) = 20 ln(4)/ ln 2 = 40 min. 2