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Lecture Notes in Differential Equations - Bruce E. Shapiro

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71<br />

From the first of equations (9.52),<br />

∫<br />

M(t, y) =<br />

N t (t, y)dy + h ′ (t) (9.61)<br />

hence<br />

∫<br />

h ′ (t) = M(t, y) −<br />

N t (t, y)dy (9.62)<br />

Multiply by dt and <strong>in</strong>tegrate,<br />

∫<br />

h(t) = h ′ (t)dt =<br />

∫ ( ∫<br />

M(t, y) −<br />

)<br />

N t (t, y)dy dt (9.63)<br />

From (9.59)<br />

∫<br />

φ(t, y) =<br />

∫ ( ∫<br />

N(t, y)dy + M(t, y) −<br />

)<br />

N t (t, y)dy dt (9.64)<br />

The follow<strong>in</strong>g theorem summarizes the derivation.<br />

Theorem 9.2. If M(t, y)dt + N(t, y)dy = 0 is exact, i.e., if<br />

∂M(t, y)<br />

∂y<br />

=<br />

∂N(t, y)<br />

∂t<br />

(9.65)<br />

The φ(t, y) = C is a solution of the ODE, where either of the follow<strong>in</strong>g<br />

formulas can be used for φ:<br />

∫<br />

∫ ( ∫<br />

)<br />

φ(t, y) = M(t, y)dt + N(t, y) − M y (t, y)dt dy (9.66)<br />

∫<br />

∫ ( ∫ )<br />

φ(t, y) = N(t, y)dy + M(t, y) − N t (t, y)dy dt (9.67)<br />

In practice, however, it is generally easier to repeat the derivation rather<br />

than memoriz<strong>in</strong>g the formula.<br />

Example 9.3. Solve<br />

This has the form M(t, y)dt + N(t, y)dy where<br />

Check<strong>in</strong>g that it is exact,<br />

(t + 2y)dt + (2t − y)dy = 0 (9.68)<br />

M(t, y) = t + 2y (9.69)<br />

N(t, y) = 2t − y (9.70)<br />

M y (t, y) = 2 = N t (t, y) (9.71)

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