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Field · Emerged 1821 – 1902

Real Analysis

What exactly are limits, continuity and the real numbers, and why did calculus need them defined?

5 chapters4 min read5 turning points0 open problems

Branched from
Calculus + Fourier Analysis
Branched into
Continuous Optimisation + Ergodic Theory + Probability Theory + Set Theory + Stochastic Processes
Figures
Augustin-Louis Cauchy, Bernard Bolzano, Bernhard Riemann, Karl Weierstrass, Richard Dedekind, Georg Cantor, Henri Lebesgue

In brief

Real analysis is calculus rebuilt on precise definitions. Instead of infinitely small quantities, it uses limits, defined by a game of tolerances: for every accuracy you demand, there is a point beyond which the values stay that close. Continuity, derivatives, integrals and infinite series are all defined this way, and so, finally, are the real numbers themselves.

It was forced into existence by failures. Intuition said every continuous curve has a slope somewhere, that series of continuous functions stay continuous, and that every function worth studying has an integral. Each turned out to be false. What came out of the repair (rigorous proof, set theory, measure) became the foundation of modern mathematics.

Key ideas

Limit (ε–δ)Enters 1821

lim⁡x→af(x)=L\lim_{x \to a} f(x) = L means: for every ε>0\varepsilon > 0 there is a δ>0\delta > 0 such that ∣f(x)−L∣<ε|f(x) - L| < \varepsilon whenever 0<∣x−a∣<δ0 < |x - a| < \delta. Infinitesimals are replaced by a precise promise.

ContinuityEnters 1872

A function is continuous if small changes in input give small changes in output, defined with limits. Continuity does not imply smoothness, as Weierstrass showed.

Completeness of the real numbersEnters 1872 – 1874

The real number line has no gaps: every bounded increasing sequence has a limit. Dedekind and Cantor constructed the reals from the rationals to guarantee it.

Uniform convergenceEnters 1821

A sequence of functions converging at the same rate everywhere, strong enough to guarantee that limits of continuous functions stay continuous. Ordinary pointwise convergence is not.

Measure and the Lebesgue integralEnters 1902

A way to assign a size to very general sets, and an integral built on it that handles far wilder functions and limits than Riemann's. It is the modern standard.

Chapter I

Answering Berkeley

For a century after Berkeley's attack, calculus ran on results rather than foundations. What changed that was teaching. At the École Polytechnique, Augustin-Louis Cauchy had to explain calculus to engineering students, and his Cours d'analyse (1821) tried to prove everything. It defined a limit as a value that quantities approach as closely as desired, a continuous function as one where small changes in input give small changes in output, and an infinite series as convergent when its partial sums settle down. The ghosts of departed quantities were replaced by statements about arbitrarily small, but always finite, numbers.

In Prague, the priest-philosopher Bernard Bolzano had reached similar definitions a few years earlier, in pamphlets almost no one read. Whether Cauchy saw them is still argued.

Chapter II

Fourier's Pressure

What made rigour urgent was Fourier analysis. Fourier series produced functions with jumps and corners as limits of smooth waves, contradicting a theorem in Cauchy's own book that limits of continuous functions are continuous. To say which functions have Fourier series, Riemann had to define the integral itself, in 1854. To say where a Fourier series could fail, Cantor was led to study strange infinite sets of points.

Then came the counterexamples. In 1872 Karl Weierstrass, who taught analysis in Berlin with ε and δ exactly as students learn it today, presented a function that is continuous everywhere and has a slope nowhere: a curve that is all corners. Charles Hermite wrote of turning away "with fright and horror from this lamentable plague of continuous functions which do not have derivatives". The lesson was blunt. Geometric intuition had misled the best mathematicians for two centuries, and only precise definitions could be trusted.

Chapter III

What Is a Real Number?

Limits need something to converge to. If the number line had gaps, a sequence could close in on a hole. Nobody had defined the real numbers; everyone had assumed them. In 1872 Richard Dedekind and Georg Cantor independently constructed them from the rationals, Dedekind by cutting the rational line into two pieces, Cantor by sequences that bunch together. Two years later Cantor proved that the real numbers cannot be listed one by one: there are strictly more of them than whole numbers. Infinity came in different sizes, and set theory was born.

Chapter IV

A Closer Look: When Intuition About Limits Fails

Cauchy's Cours d'analyse stated that a convergent series of continuous functions is continuous. Here is why that is false. Take the functions fn(x)=xnf_n(x) = x^n on the interval [0,1][0, 1]. Each is continuous, a smooth curve. As nn grows, for any x<1x < 1 the values xnx^n shrink to 0, while at x=1x = 1 they stay at 1. The limit is

f(x)={00≤x<1,1x=1,f(x) = \begin{cases} 0 & 0 \le x < 1, \\ 1 & x = 1, \end{cases}

which jumps. Continuous functions converged, point by point, to a discontinuous one.

The repair is uniform convergence: require that a single nn make fnf_n close to ff at every xx at once. Here that fails. However large nn is, points just below 1 still have xnx^n near 1, far from the limit 0. Seidel, Stokes and Weierstrass showed that uniform limits of continuous functions are continuous, and the distinction between the two kinds of convergence became basic analysis.

Precise definitions are what make such distinctions possible. The statement lim⁡x→2x2=4\lim_{x \to 2} x^2 = 4 means: for every tolerance ε>0\varepsilon > 0 there is a δ>0\delta > 0 such that ∣x2−4∣<ε|x^2 - 4| < \varepsilon whenever ∣x−2∣<δ|x - 2| < \delta. To prove it, factor ∣x2−4∣=∣x−2∣ ∣x+2∣|x^2 - 4| = |x - 2|\,|x + 2|. If ∣x−2∣<1|x - 2| < 1 then ∣x+2∣<5|x + 2| < 5, so ∣x2−4∣<5∣x−2∣|x^2 - 4| < 5|x - 2|. Choosing

δ=min⁡ ⁣(1,ε5)\delta = \min\!\left(1, \frac{\varepsilon}{5}\right)

guarantees ∣x2−4∣<ε|x^2 - 4| < \varepsilon. No infinitesimals are involved, only finite numbers and a promise that holds for every tolerance. That is the whole of Weierstrass's answer to Berkeley.

Chapter V

Measure

The last repair was to the integral. Riemann's integral cannot handle Dirichlet's function (1 on rationals, 0 on irrationals), and it behaves badly under limits. In 1902 Henri Lebesgue built a new one on a theory of measure, a consistent way of assigning size to very general sets. He compared it to counting money. Riemann adds up coins in the order he picks them up, while Lebesgue first sorts them by value. Measure theory became the foundation of modern analysis, and thirty years later the foundation of probability too.

Open problems

Where the map runs out

No open problems are recorded here. This field's unanswered questions moved into its successors: Continuous Optimisation + Ergodic Theory + Probability Theory + Set Theory + Stochastic Processes.

Further reading

  1. Bressoud, D. M. (2007). A Radical Approach to Real Analysis (2nd ed.). Mathematical Association of America.

    Teaches the subject through the Fourier-series crisis that created it. The ideal companion to this page.

  2. Abbott, S. (2015). Understanding Analysis (2nd ed.). Springer.

    A friendly, well-motivated first course in rigorous analysis.

  3. Grabiner, J. V. (1981). The Origins of Cauchy's Rigorous Calculus. MIT Press.

    How the ε–δ definitions came to be.