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@jemoka / Jemoka Knowledge Base / raw/concept/kbhseperable_diffequ.md
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--- title: "seperable diffequ" source: https://www.jemoka.com/posts/kbhseperable_diffequ/ --- \begin{equation} \dv{y}{t} = a(t)f(y) \end{equation} are a class of functions are called seperable. We can solve them using the division method division method the division method involves solving autonomous ODEs by dividing and treating it normally: \begin{equation} y’ = 8y \end{equation} \begin{equation} \frac{y’}{8} = y \end{equation} we now write something fishy: \begin{equation} \frac{\dd{y}}{y} = 8 \dd{t} \end{equation} we now take the antiderivative of this: \begin{equation} \int \frac{1}{y} \dd{y} = \int 8 \dd{t} \end{equation} We will get that: \begin{equation} \ln |y| = 8t + C \end{equation} we finally get: \begin{equation} |y| = e^{C} e^{8t} \end{equation} getting rid of that absolute value: \begin{align} y &= \pm e^{C} e^{8t} \\ &= K e^{8t} \end{align} places where this breaks down sometimes, \(\frac{1}{f(y)}\) may not have a nice antiderivative sometimes, \(G(y)\), the antidepressant, may not be nicely invertible general solution to y’(t) = ry(t) generally, for \(r \in \mathbb{R}\), the solution to \(y’(t) = ry(t)\) is at \(y(t)=y_0e^{rt}\), where \(y_0 = y(0)\). for autonomous ODEs for which \(ry(t) = f(y)\), we have that: \begin{equation} \dv{y}{x} = ry(x) \end{equation} which means: \begin{equation} \frac{1}{y(x)} \dd{y} = r\dd{x} \end{equation} and so: \begin{equation} \ln \qty| y(x) | = rx +C \end{equation} and hence: \begin{equation} y(x) = K e^{rx} \end{equation} plugging in \(x=0\), yields \(y(0) = Ke^{0} = K\).