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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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Lesson 10<br />

Integrat<strong>in</strong>g Factors<br />

Def<strong>in</strong>ition 10.1. An <strong>in</strong>tegrat<strong>in</strong>g factor for the differential equation<br />

is a any function such µ(t, y) such that<br />

is exact.<br />

M(t, y)dt + N(t, y)dy = 0 (10.1)<br />

µ(t, y)M(t, y)dt + µ(t, y)N(t, y)dy = 0 (10.2)<br />

If (10.2) is exact, then by theorem 9.1<br />

∂<br />

∂y (µ(t, y)M(t, y)) = ∂ (µ(t, y)N(t, y)) (10.3)<br />

∂t<br />

In this section we will discuss some special cases <strong>in</strong> which we can solve (10.3)<br />

to f<strong>in</strong>d an <strong>in</strong>tegrat<strong>in</strong>g factor µ(t, y) that satisfies (10.3). First we give an<br />

example to that demonstrates how we can use an <strong>in</strong>tegrat<strong>in</strong>g factor.<br />

Example 10.1. Show that<br />

( ) ( s<strong>in</strong> y<br />

cos y + 2e<br />

− 2e −t −t )<br />

cos t<br />

s<strong>in</strong> t dt +<br />

dy = 0 (10.4)<br />

y<br />

y<br />

is not exact, and then show that<br />

µ(t, y) = ye t (10.5)<br />

is an <strong>in</strong>tegrat<strong>in</strong>g factor for (10.4), and then use the <strong>in</strong>tegrat<strong>in</strong>g factor to<br />

f<strong>in</strong>d a general solution of (10.4).<br />

77

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