First Order ODE/(sine x sine y - x e^y) dy = (e^y + cosine x cosine y) dx
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Theorem
The first order ordinary differential equation:
- $(1): \quad \paren {\sin x \sin y - x e^y} \rd y = \paren {e^y + \cos x \cos y} \rd x$
is an exact differential equation with solution:
- $\sin x \cos y + x e^y = C$
This can also be presented as:
- $\dfrac {\d y} {\d x} = \dfrac {e^y + \cos x \cos y} {\sin x \sin y - x e^y}$
Proof
First express $(1)$ in the form:
- $(2): \quad -\paren {e^y + \cos x \cos y} + \paren {\sin x \sin y - x e^y} \dfrac {\d y} {\d x}$
Let:
- $\map M {x, y} = -\paren {e^y + \cos x \cos y}$
- $\map N {x, y} = \sin x \sin y - x e^y$
Then:
\(\ds \dfrac {\partial M} {\partial y}\) | \(=\) | \(\ds -e^y + \cos x \sin y\) | ||||||||||||
\(\ds \dfrac {\partial N} {\partial x}\) | \(=\) | \(\ds -e^y + \cos x \sin y\) |
Thus $\dfrac {\partial M} {\partial y} = \dfrac {\partial N} {\partial x}$ and $(1)$ is seen by definition to be exact.
By Solution to Exact Differential Equation, the solution to $(1)$ is:
- $\map f {x, y} = C$
where:
\(\ds \dfrac {\partial f} {\partial x}\) | \(=\) | \(\ds \map M {x, y}\) | ||||||||||||
\(\ds \dfrac {\partial f} {\partial y}\) | \(=\) | \(\ds \map N {x, y}\) |
Hence:
\(\ds f\) | \(=\) | \(\ds \map M {x, y} \rd x + \map g y\) | ||||||||||||
\(\ds \) | \(=\) | \(\ds -\int \paren {e^y + \cos x \cos y} \rd x + \map g y\) | ||||||||||||
\(\ds \) | \(=\) | \(\ds -x e^y - \sin x \cos y + \map g y\) |
and:
\(\ds f\) | \(=\) | \(\ds \int \map N {x, y} \rd y + \map h x\) | ||||||||||||
\(\ds \) | \(=\) | \(\ds \int \paren {\sin x \sin y - x e^y} \rd y + \map h x\) | ||||||||||||
\(\ds \) | \(=\) | \(\ds -\sin x \cos y - x e^y + \map h x\) |
Thus:
- $\map f {x, y} = -\sin x \cos y - x e^y$
and by Solution to Exact Differential Equation, the solution to $(1)$, after simplification, is:
- $\sin x \cos y + x e^y = C$
$\blacksquare$
Sources
- 1972: George F. Simmons: Differential Equations ... (previous) ... (next): $\S 2.8$: Exact Equations: Problem $7$