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References and credits

Further reading Cajori, Florian. A History of Mathematical Notations. 2 vols. Chicago: Open Court, 1928–1929. The notations of Newton, Leibniz, Lagrange and Arbogast, the $\int$ and Fourier’s limits, Wallis’s $\infty$. Lagrange, Joseph-Louis. Théorie des fonctions analytiques. Paris: Imprimerie de la République, 1797. Arbogast, Louis F. A. Du calcul des dérivations. Strasbourg: Levrault, 1800. Wallis, John. De sectionibus conicis. Oxford, 1655. And Arithmetica infinitorum. Oxford, 1656. Boole, George. On a general method in analysis. Philosophical Transactions of the Royal Society, 134, 1844, pp. 225–282. Heaviside, Oliver. Electromagnetic Theory. 3 vols. London: The Electrician, 1893–1912. Child, J. M. The Early Mathematical Manuscripts of Leibniz. Chicago: Open Court, 1920. The manuscripts of October 1675, with “omn.” and the first $\int$. Robinson, Abraham. Non-standard Analysis. Amsterdam: North-Holland, 1966. Tall, David; Vinner, Shlomo. Concept image and concept definition in mathematics with particular reference to limits and continuity. Educational Studies in Mathematics, 12, 1981, pp. 151–169. Thompson, Silvanus P. Calculus Made Easy. London: Macmillan, 1910. The book that teaches calculus by treating $dx$ as “a little bit of $x$”. Earliest Uses of Symbols of Calculus, Jeff Miller. Image sources Image Source Licence Title page of Lagrange’s Théorie des fonctions analytiques (1797) Wikimedia Commons public domain Oliver Heaviside, portrait by an unknown author Wikimedia Commons public domain The first use of the sign ∞, Wallis’s De sectionibus conicis (1655) Wikimedia Commons public domain John Wallis, portrait after Godfrey Kneller Wikimedia Commons public domain The interactive figures (the secant that becomes a tangent and the Riemann sums) were produced for this book and work in all four languages of the site. The record of the downloaded images, with the hash of each file, is in data/semiotica_imagens.json.

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How to read calculus: a guide and a glossary

This chapter read the signs of calculus one by one. The guide below gathers the questions that help read them together. Five questions for calculus What varies, and with respect to what? In $\frac{dy}{dx}$, both letters are written. In $f'$, the variable is implicit; in $\dot x$, it is time. If it is not clear, write it down. Is it a finite difference or a limit? $\Delta$ and $\Sigma$ are calculations with numbers; $d$ and $\int$ are what remains when the calculation shrinks without end. The shape looks alike; the meaning changes. Does cancelling hold here? With one variable and one order of differentiation, $\frac{dy}{dx}$ behaves like a fraction. With second derivatives or partial derivatives, check before cancelling. Which letter is a dummy? In the integral, the letter of the $d$ is bound; in the limit, the letter of the arrow is too. Neither may appear outside. Is the $\infty$ a direction or a quantity? In $x\to\infty$ and $\sum^\infty$, it is a direction, and calculations with it need a limit. Only Cantor’s $\aleph$s are quantities. A complete reading of an equation $$\frac{d}{dx}\int_0^{x}e^{-t^2}\,dt=e^{-x^2}.$$ The integral $\int_0^xe^{-t^2}\,dt$ is the area under the bell-shaped curve, from $0$ to $x$. It is a function of $x$: each $x$ gives an area. The $t$ is a dummy letter. Replacing it with $s$ changes nothing. Replacing it with $x$ would be a mistake, because $x$ is already in the limit. The $\frac{d}{dx}$ is an operator: it asks for the rate at which that area grows as $x$ grows. The $=$ states an identity, valid for every $x$. It is the first part of the fundamental theorem. The remarkable detail: the integral $\int_0^xe^{-t^2}\,dt$ has no formula in elementary functions. Even so, its derivative is written in one line. The notation lets you talk about a function without knowing how to write it. Glossary Difference ($\Delta$). Finite change in a quantity: $\Delta y=f(x+\Delta x)-f(x)$. Differential ($dy$). Change along the tangent line: $dy=f'(x)\,dx$. Approximates $\Delta y$ when the step is small. Derivative. Limit of $\frac{\Delta y}{\Delta x}$ as $\Delta x\to0$. Written $\frac{dy}{dx}$, $f'(x)$, $\dot y$ or $Dy$. Operator. Rule that turns one function into another, such as $D$, which differentiates. It can be added, multiplied and, with care, factorised. Characteristic equation. Polynomial obtained by replacing $D$ with $r$ in a linear differential equation with constant coefficients. Riemann sum. Sum $\sum f(x_i)\,\Delta x$ of areas of rectangles that approximate an integral. Definite integral. Limit of the Riemann sums: $\int_a^b f(x)\,dx$, a number. Antiderivative (indefinite integral). Function $F$ with $F'=f$. Determined up to a constant: $\int f(x)\,dx=F(x)+C$. Fundamental theorem of calculus. Differentiating and integrating are inverse operations: $\frac{d}{dx}\int_a^xf=f(x)$ and $\int_a^bF'=F(b)-F(a)$. Indeterminate form. Expression such as $\infty-\infty$ or $\frac00$ whose value depends on the route, not only on the form. Series. Sum with infinitely many terms. It converges when the partial sums approach a number, which is called the sum of the series. Conditional convergence. Series that converges, but whose sum changes when the terms are rearranged. Exercise: apply the guideRead $\displaystyle\lim_{h\to0}\frac{\sin(x+h)-\sin x}{h}=\cos x$. What varies is $h$, bound by the limit; $x$ is free. The fraction is a finite difference divided by the step, $\frac{\Delta y}{\Delta x}$, and the limit turns it into the derivative. The $=$ is an identity, valid for every $x$. In Lagrange’s notation, it is the sentence $\sin'=\cos$; in Arbogast’s, $D\sin=\cos$.