Skip to main content\(\newcommand\DLGray{\color{Gray}}
\newcommand\DLO{\color{BurntOrange}}
\newcommand\DLRa{\color{WildStrawberry}}
\newcommand\DLGa{\color{Green}}
\newcommand\DLGb{\color{PineGreen}}
\newcommand\DLBa{\color{RoyalBlue}}
\newcommand\DLBb{\color{Cerulean}}
\newcommand\ds{\displaystyle}
\newcommand\ddx{\frac{d}{dx}}
\newcommand\os{\overset}
\newcommand\us{\underset}
\newcommand\ob{\overbrace}
\newcommand\obt{\overbracket}
\newcommand\ub{\underbrace}
\newcommand\ubt{\underbracket}
\newcommand\ul{\underline}
\newcommand\laplacesym{\mathscr{L}}
\newcommand\lap[1]{\laplacesym\left\{#1\right\}}
\newcommand\ilap[1]{\laplacesym^{-1}\left\{#1\right\}}
\newcommand\tikznode[3][]
{\tikz[remember picture,baseline=(#2.base)]
\node[minimum size=0pt,inner sep=0pt,#1](#2){#3};
}
\newcommand{\lt}{<}
\newcommand{\gt}{>}
\newcommand{\amp}{&}
\definecolor{fillinmathshade}{gray}{0.9}
\newcommand{\fillinmath}[1]{\mathchoice{\colorbox{fillinmathshade}{$\displaystyle \phantom{\,#1\,}$}}{\colorbox{fillinmathshade}{$\textstyle \phantom{\,#1\,}$}}{\colorbox{fillinmathshade}{$\scriptstyle \phantom{\,#1\,}$}}{\colorbox{fillinmathshade}{$\scriptscriptstyle\phantom{\,#1\,}$}}}
\newcommand{\sfrac}[2]{{#1}/{#2}}
\)
๐๏ธ Key Takeaways ...
-
In uncoupled systems,
-
there is no interaction between equations,
-
each variable evolves independently, and
These are the simplest systems โ but theyโre still systems!
-
In partially-coupled systems,
-
one equation is independent, and the other depends on it,
-
You can solve these without any new ideas by solving the independent equation first, then substituting its solution into the dependent equation.
These systems model one-way influences, like a light level driving plant growth.
-
The most common systems are fully-coupled systems, where
-
both variables influence each other, and
-
neither equation can be solved in isolation. That is, the system must be treated as a whole.
-
A system is linear if its unknowns appear without products, powers, or nonlinear functions. Such systems can be written in vector form:
\begin{equation*}
\dfrac{d\vec{X}}{dt} = A\vec{X}
\end{equation*}
where \(A\) is the constant coefficient matrix.
-
Solving such systems is an eigenvalue problem.
-
Eulerโs Method updates each variable using its derivative at the current step. This update feeds into the coupled variables.
-
Phase plane diagrams reveal whether a systemโs solutions decay, grow, or spiral.
-
You can often tell what will happen by the shape of the arrows โ even without solving equations.