The spring and differential equations
A differential equation is an equation in which the unknown is a function, and the equation speaks of its derivatives. Euler organized this path into a scheme that we still use today: observe a phenomenon, write the equation, find the function that solves it and draw the graph.
flowchart LR phenomenon((FENÔMENO)) --> equation["EQUAÇÃODIFERENCIAL"] equation --> solution["FUNÇÃOSOLUÇÃO"] solution --> plottedGraph((GRÁFICO)) plottedGraph --> derivative{"DERIVADA"} derivative --> phenomenon derivative -. "localiza" .-> extrema["Pontos de máximoe de mínimo"] classDef phenomenonStyle fill:#e6f1ee,stroke:#397c75,color:#243448,stroke-width:2px classDef equationStyle fill:#eaf0f7,stroke:#58799b,color:#243448,stroke-width:2px classDef solutionStyle fill:#f8efd9,stroke:#b68b3c,color:#243448,stroke-width:2px classDef derivativeStyle fill:#f5e9e3,stroke:#9b6251,color:#243448,stroke-width:2px class phenomenon phenomenonStyle class equation,plottedGraph equationStyle class solution solutionStyle class derivative,extrema derivativeStyle The phenomenon. In 1678, Robert Hooke summarized the behavior of a spring in Latin: ut tensio, sic vis, “as extension, so strength.” A spring of constant $k$, stretched by $x$, pulls back with strength $F = -kx$.