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Lecture Notes in Differential Equations - Bruce E. Shapiro

Lecture Notes in Differential Equations - Bruce E. Shapiro

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82 LESSON 10. INTEGRATING FACTORS<br />

Rearrang<strong>in</strong>g,<br />

1 d<br />

µ(y) dy µ(y) = N t(t, y) − M y (t, y)<br />

= P (2) (y) (10.44)<br />

M(t, y)<br />

Multiply by dy and <strong>in</strong>tegrat<strong>in</strong>g,<br />

∫<br />

∫<br />

1 d<br />

µ(y) dy µ(y)dy = P (2) (y)dy (10.45)<br />

Integrat<strong>in</strong>g and exponentiat<strong>in</strong>g<br />

(∫<br />

µ(y) = exp<br />

)<br />

P (2) (y)dy<br />

(10.46)<br />

as required by equation (10.29). (Case 2).<br />

Case 3. If µ(t, y) = µ(z) is only a function of z = ty then<br />

∂z<br />

∂t = ∂(ty) = y<br />

∂t<br />

(10.47)<br />

∂z<br />

∂y = ∂(ty) = t<br />

∂y<br />

(10.48)<br />

S<strong>in</strong>ce µ(z) is only a function of a s<strong>in</strong>gle variable z we will denote<br />

µ ′ (z) = dµ<br />

dz<br />

By the cha<strong>in</strong> rule and equations (10.47),(10.48), and (10.49),<br />

Us<strong>in</strong>g these results <strong>in</strong> (10.38),<br />

(10.49)<br />

∂µ<br />

∂t = dµ ∂z<br />

dz ∂t = µ′ (z)y (10.50)<br />

∂µ<br />

∂y = du ∂z<br />

dz ∂y = µ′ (z)t (10.51)<br />

µ(z)M y (t, y) + µ ′ (z)tM(t, y) = µ(z)N t (t, y) + µ ′ (z)yN(t, y) (10.52)<br />

µ ′ (z) × (tM(t, y) − yN(t, y)) = µ(z) × (N t (t, y) − M y (t, y)) (10.53)<br />

µ ′ (z)<br />

µ(z) = N t(t, y) − M y (t, y)<br />

tM(t, y) − yN(t, y)) = P (3) (z) (10.54)<br />

Integrat<strong>in</strong>g and exponentiat<strong>in</strong>g,<br />

(∫<br />

µ(z) = exp<br />

)<br />

P (3) (z)dz<br />

(10.55)

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