Lecture Notes in Differential Equations - Bruce E. Shapiro

Lecture Notes in Differential Equations - Bruce E. Shapiro Lecture Notes in Differential Equations - Bruce E. Shapiro

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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)

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)

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