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Lecture Notes in Differential Equations - Bruce E. Shapiro

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78 LESSON 10. INTEGRATING FACTORS<br />

We are first asked to verify that (10.4) is not exact. To do this we must<br />

show that M y ≠ N x , so we calculate the partial derivatives.<br />

∂M<br />

∂y = ∂ ( )<br />

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

− 2e −t y cos t − s<strong>in</strong> y<br />

s<strong>in</strong> t =<br />

∂y y<br />

y 2 (10.6)<br />

∂N<br />

∂t = ∂ ( cos y + 2e −t )<br />

cos t<br />

= − 2 ∂t y<br />

y e−t (s<strong>in</strong> t + cos t) (10.7)<br />

S<strong>in</strong>ce M y ≠ N t we may conclude that equation (10.4) is not exact.<br />

To show that (10.5) is an <strong>in</strong>tegrat<strong>in</strong>g factor, we multiply the differential<br />

equation by µ(t, y). This gives<br />

(<br />

e t s<strong>in</strong> y − 2y s<strong>in</strong> t ) dt + ( e t cos y + 2 cos t ) dy = 0 (10.8)<br />

which is <strong>in</strong> the form M(t, y)dt + N(t, y)dy with<br />

The partial derivatives are<br />

M(t, y) = e t s<strong>in</strong> y − 2y s<strong>in</strong> t (10.9)<br />

N(t, y) = e t cos y + 2 cos t (10.10)<br />

∂M(t, y)<br />

∂y<br />

∂N(t, y)<br />

∂t<br />

= ∂ ∂y (et s<strong>in</strong> y − 2y s<strong>in</strong> t) (10.11)<br />

= e t (cos y − 2 s<strong>in</strong> t) (10.12)<br />

= ∂ ∂t (et cos y + 2 cos t) (10.13)<br />

= e t (cos y − 2 s<strong>in</strong> t) (10.14)<br />

S<strong>in</strong>ce M y = N t , we may conclude that (10.8) is exact.<br />

S<strong>in</strong>ce (10.8) is exact, its solution is φ(t, y) = C for some function φ that<br />

satisifes<br />

∂φ<br />

∂t = M(t, y) = et s<strong>in</strong> y − 2y s<strong>in</strong> t (10.15)<br />

∂φ<br />

∂y = N(t, y) = et cos y + 2 cos t (10.16)<br />

From (10.15)

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