Lecture Notes in Differential Equations - Bruce E. Shapiro
Lecture Notes in Differential Equations - Bruce E. Shapiro Lecture Notes in Differential Equations - Bruce E. Shapiro
62 LESSON 8. HOMOGENEOUS EQUATIONS The equation has the form y ′ = f(t, y) where f(t, y) = 2ty t 2 − 3y 2 (8.5) 2ty = (t 2 )(1 − 3(y/t) 2 ) (8.6) = 2(y/t) 1 − 3(y/t) 2 (8.7) = 2z 1 − 3z 2 (8.8) where z = y/t. Hence the ODE is homogeneous. The following procedure shows that any homogeneous equation can be converted to a separable equation in z by substituting z = y/t. Let z = y/t. Then y = tz and thus dy dt = d (tz) = tdz dt dt + z (8.9) Thus if dy ( y ) dt = g (8.10) t then t dz + z = g(z) (8.11) dt where z = y/t. Bringing the the z to the right-hand side, t dz dt which is a separable equation in z. = g(z) − z (8.12) dz dt = g(z) − z t dz g(z) − z = dt t Example 8.2. Find the one-parameter family of solutions to (8.13) (8.14) Since y ′ = y2 + 2ty t 2 y ′ = y2 + 2ty t 2 (8.15) = y2 t 2 + 2ty ( y ) 2 t 2 = y + 2 t t = z2 + 2z (8.16)
63 where z = y/t, the differential equation is homogeneous. Hence by equation (8.12) it is equivalent to the following equation in z: Rearranging and separating variables, Integrating, Exponentiating, dt t = dz z 2 + z = t dz dt + z = z2 + 2z (8.17) t dz dt = z2 + z (8.18) ( dz 1 z(1 + z) = z − 1 ) dz (8.19) 1 + z ∫ ∫ ∫ dt dz t = z − dz (8.20) 1 + z ln |t| = ln |z| − ln |1 + z| + C = ln z ∣1 + z ∣ + C (8.21) t = C′ z (8.22) 1 + z for some new constant C’. Dropping the prime on the C and rearranging to solve for z, (1 + z)t = Cz (8.23) t = Cz − zt = z(C − t) (8.24) z = t C − t Since we started the whole process by substituting z = y/t then (8.25) y = zt = t2 C − t as the general solution of the original differential equation. Example 8.3. Solve the initial value problem dy dt = y ⎫ t − 1 ⎬ ⎭ y(1) = 2 (8.26) (8.27) Letting z = y/t the differential equation becomes dy dt = z − 1 (8.28)
- Page 19 and 20: Lesson 2 A Geometric View One way t
- Page 21 and 22: 13 We can extend this geometric int
- Page 23 and 24: 15 that since the slope of the solu
- Page 25 and 26: Lesson 3 Separable Equations An ODE
- Page 27 and 28: 19 Since it is not possible to solv
- Page 29 and 30: 21 where M(t) = −a(t) and N(y) =
- Page 31 and 32: 23 Example 3.10. Find a general sol
- Page 33 and 34: Lesson 4 Linear Equations Recall th
- Page 35 and 36: 27 So far any function µ will work
- Page 37 and 38: 29 Example 4.1. Solve the different
- Page 39 and 40: 31 Since p(t) = 1 (the coefficient
- Page 41 and 42: 33 Multiplying equation 4.68 by µ
- Page 43 and 44: 35 Substituting y = t = 0 in this i
- Page 45 and 46: 37 ∫ t t 0 Evaluating the integra
- Page 47 and 48: Lesson 5 Bernoulli Equations The Be
- Page 49 and 50: 41 This is a Bernoulli equation wit
- Page 51 and 52: Lesson 6 Exponential Relaxation One
- Page 53 and 54: 45 Exponential Runaway First we con
- Page 55 and 56: 47 Figure 6.2: Illustration of the
- Page 57 and 58: 49 This is identical to with Theref
- Page 59 and 60: 51 this becomes a first-order ODE i
- Page 61 and 62: Lesson 7 Autonomous Differential Eq
- Page 63 and 64: 55 Figure 7.1: A plot of the right-
- Page 65 and 66: 57 Figure 7.2: Solutions of the log
- Page 67 and 68: 59 Figure 7.4: Solutions of the thr
- Page 69: Lesson 8 Homogeneous Equations Defi
- Page 73 and 74: Lesson 9 Exact Equations We can re-
- Page 75 and 76: 67 Now compare equation (9.2) with
- Page 77 and 78: 69 Hence dg dy = 0 =⇒ g = C′ (9
- Page 79 and 80: 71 From the first of equations (9.5
- Page 81 and 82: 73 Differentiating equations (9.81)
- Page 83 and 84: 75 This has the form Mdt + Ndy = 0
- Page 85 and 86: Lesson 10 Integrating Factors Defin
- Page 87 and 88: 79 Differentiating with respect to
- Page 89 and 90: 81 Proof. In each of the five cases
- Page 91 and 92: 83 as required by equation (10.31).
- Page 93 and 94: 85 Since M y ≠ N t , equation (10
- Page 95 and 96: 87 the revised equation (10.100) is
- Page 97 and 98: 89 Substituting (10.129) into (10.1
- Page 99 and 100: Lesson 11 Method of Successive Appr
- Page 101 and 102: 93 because the integral is zero (th
- Page 103 and 104: 95 Example 11.1. Construct the Pica
- Page 105 and 106: 97 We can then plug this expression
- Page 107 and 108: Lesson 12 Existence of Solutions* I
- Page 109 and 110: 101 • Interchangeability of Limit
- Page 111 and 112: 103 But on the square −1 ≤ t
- Page 113 and 114: 105 Thus lim φ n = φ 0 + lim n→
- Page 115 and 116: 107 because the right hand side doe
- Page 117 and 118: Lesson 13 Uniqueness of Solutions*
- Page 119 and 120: 111 The proof of theorem (13.1) is
63<br />
where z = y/t, the differential equation is homogeneous. Hence by equation<br />
(8.12) it is equivalent to the follow<strong>in</strong>g equation <strong>in</strong> z:<br />
Rearrang<strong>in</strong>g and separat<strong>in</strong>g variables,<br />
Integrat<strong>in</strong>g,<br />
Exponentiat<strong>in</strong>g,<br />
dt<br />
t =<br />
dz<br />
z 2 + z =<br />
t dz<br />
dt + z = z2 + 2z (8.17)<br />
t dz<br />
dt = z2 + z (8.18)<br />
(<br />
dz 1<br />
z(1 + z) = z − 1 )<br />
dz (8.19)<br />
1 + z<br />
∫ ∫ ∫<br />
dt dz<br />
t = z − dz<br />
(8.20)<br />
1 + z<br />
ln |t| = ln |z| − ln |1 + z| + C = ln<br />
z<br />
∣1 + z ∣ + C (8.21)<br />
t = C′ z<br />
(8.22)<br />
1 + z<br />
for some new constant C’. Dropp<strong>in</strong>g the prime on the C and rearrang<strong>in</strong>g<br />
to solve for z,<br />
(1 + z)t = Cz (8.23)<br />
t = Cz − zt = z(C − t) (8.24)<br />
z =<br />
t<br />
C − t<br />
S<strong>in</strong>ce we started the whole process by substitut<strong>in</strong>g z = y/t then<br />
(8.25)<br />
y = zt =<br />
t2<br />
C − t<br />
as the general solution of the orig<strong>in</strong>al differential equation.<br />
Example 8.3. Solve the <strong>in</strong>itial value problem<br />
dy<br />
dt = y ⎫<br />
t − 1 ⎬<br />
⎭<br />
y(1) = 2<br />
(8.26)<br />
(8.27)<br />
Lett<strong>in</strong>g z = y/t the differential equation becomes<br />
dy<br />
dt = z − 1 (8.28)