First Order ODE/y' - f (y) phi' (x) over f' (y) = phi (x) phi' (x) over f' (y)
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Theorem
Let $\map f y$ and $\map \phi x$ be known real functions of $y$ and $x$ respectively.
The general solution of:
- $(1): \quad \dfrac {\d y} {\d x} - \dfrac {\map f y} {\map {f'} y} \map {\phi'} x = \dfrac {\map \phi x \map {\phi'} x} {\map {f'} y}$
is:
- $\map f y = C e^{\map \phi x} - \map \phi x - 1$
Proof
Let $u = \map f y$
Then by the Chain Rule for Derivatives:
- $\dfrac {\d u} {\d x} = \map {f'} y \dfrac {\d y} {\d x}$
Then:
\(\ds \dfrac {\d y} {\d x} - \dfrac {\map f y} {\map {f'} y} \map {\phi'} x\) | \(=\) | \(\ds \dfrac {\map \phi x \map {\phi'} x} {\map {f'} y}\) | ||||||||||||
\(\ds \leadsto \ \ \) | \(\ds \map {f'} y \dfrac {\d y} {\d x} - \map f y \map {\phi'} x\) | \(=\) | \(\ds \map \phi x \map {\phi'} x\) | multiplying $(1)$ by $\map {f'} y$ | ||||||||||
\(\ds \leadsto \ \ \) | \(\ds \dfrac {\d u} {\d x} - u \map {\phi'} x\) | \(=\) | \(\ds \map \phi x \map {\phi'} x\) | substituting $u$ for $\map f y$ |
This is a linear first order ordinary differential equation in the form:
- $\dfrac {\d u} {\d x} + \map P x u = \map Q x$
whose general solution from Solution to Linear First Order Ordinary Differential Equation is:
- $\ds u e^{\int P \rd x} = \int Q e^{\int P \rd x} \rd x + C$
In this instance:
- $\map P x = -\map {\phi'} x$
and:
- $\map Q x = \map \phi x \map {\phi'} x$
Thus:
\(\ds \int P \rd x\) | \(=\) | \(\ds -\int \map {\phi'} x \rd x\) | ||||||||||||
\(\ds \) | \(=\) | \(\ds -\map \phi x + A\) |
Hence:
- $\ds u e^{-\map \phi x + A} = \int \map \phi x \map {\phi'} x e^{-\map \phi x + A} \rd x + C$
Let $v = \map \phi x$.
Then by Integration by Substitution:
\(\ds \int \map \phi x \map {\phi'} x e^{-\map \phi x + A} \rd x\) | \(=\) | \(\ds \int v e^{-v + A} \rd v\) | Integration by Substitution | |||||||||||
\(\ds \) | \(=\) | \(\ds \int v e^{-v} e^A \rd v\) | ||||||||||||
\(\ds \) | \(=\) | \(\ds e^A \int v e^{-v} \rd v\) | ||||||||||||
\(\ds \) | \(=\) | \(\ds - e^A e^{-v} \paren {v + 1} + C'\) | Primitive of $x e^{a x}$ |
This leaves us with:
- $u e^{-\map \phi x + A} = - e^A e^{-v} \paren {v + 1} + C$
subsuming $C'$ into $C$.
Substituting back in, the general solution is seen to be:
- $\map f y e^{-\map \phi x + A} = - e^{-\map \phi x + A} \paren {\map \phi x + 1} + C$
and so multiplying both sides by $e^{\map \phi x - A}$:
\(\ds \map f y\) | \(=\) | \(\ds \paren {-\map \phi x - 1} + C e^{\map \phi x - A}\) | ||||||||||||
\(\ds \) | \(=\) | \(\ds C e^{-A} e^{\map \phi x} - \map \phi x - 1\) | ||||||||||||
\(\ds \) | \(=\) | \(\ds C e^{\map \phi x} - \map \phi x - 1\) | by absorbing the constant factor $e^{-A}$ into $C$ |
Hence the result.
$\blacksquare$
Sources
- 1896: Joseph Edwards: Integral Calculus for Beginners: With an Introduction to the Study of Differential Equations: Exercise $18 \ (4)$