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The Timpson Lyceum · Real Analysis (2020)

Lecture 18 (Real Analysis 2020)

Overview

This lecture develops the central tool for deciding when a bounded function can be integrated: the Archimedes–Riemann theorem. It characterizes integrability in terms of a sequence of partitions whose upper and lower Darboux sums close the gap to zero, and uses this to prove that every monotonic function on a closed interval is integrable. Along the way it introduces regular partitions and the gap (mesh) of a partition, and closes with a fully worked computation of ∫01x2 dx\int_0^1 x^2\,dx from the definition. The recurring strategy — show the difference of upper and lower sums tends to zero — is the workhorse for the rest of the chapter. A short final discussion connects this picture to Leibniz notation and the way integrals are introduced in a standard calculus course.

Key Concepts

Setup and the Darboux integral. Throughout, f:[a,b]→Rf:[a,b]\to\mathbb{R} is bounded (a necessary hypothesis — an unbounded function cannot enclose a finite area). The lower integral ∫ab‾f\underline{\int_a^b} f is the supremum (least upper bound) of all lower Darboux sums; the upper integral ∫ab‾f\overline{\int_a^b} f is the infimum (greatest lower bound) of all upper Darboux sums. The function is integrable exactly when these agree, and the common value is the integral:

∫ab‾f  =  ∫ab‾f  =:  ∫abf.\underline{\int_a^b} f \;=\; \overline{\int_a^b} f \;=:\; \int_a^b f.

The sandwiching inequality. For any partitions, the lower sum, lower integral, upper integral, and upper sum are ordered:

L(f,P)  ≤  ∫ab‾f  ≤  ∫ab‾f  ≤  U(f,Q).L(f,P) \;\le\; \underline{\int_a^b} f \;\le\; \overline{\int_a^b} f \;\le\; U(f,Q).

A useful rearrangement: U(f,Q)−L(f,P)≥∫‾f−∫‾f≥0U(f,Q) - L(f,P) \ge \overline{\int} f - \underline{\int} f \ge 0. Because both differences are nonnegative, driving the outer difference to zero forces the inner one to zero as well — this is why the theorem below works.

Archimedes–Riemann theorem. A bounded f:[a,b]→Rf:[a,b]\to\mathbb{R} is integrable if and only if there exists a sequence of partitions (Pn)(P_n) with

lim⁡n→∞(U(f,Pn)−L(f,Pn))=0.\lim_{n\to\infty}\bigl(U(f,P_n) - L(f,P_n)\bigr) = 0.

Such a sequence is called an Archimedean sequence of partitions. Moreover, when it exists, lim⁡n→∞L(f,Pn)=∫‾f\lim_{n\to\infty} L(f,P_n) = \underline{\int} f and lim⁡n→∞U(f,Pn)=∫‾f\lim_{n\to\infty} U(f,P_n) = \overline{\int} f. Note carefully: the theorem certifies that an integral exists; it does not by itself compute its value.

Regular partition. Splitting [a,b][a,b] into nn equal pieces. The ii-th partition point is

xi=a+i b−an,0≤i≤n,x_i = a + i\,\frac{b-a}{n}, \qquad 0 \le i \le n,

so each subinterval has the same width b−an\dfrac{b-a}{n}. Regular partitions are the easiest to compute with by hand, but the theorem does not require them.

Gap (mesh) of a partition. The gap of PP is the length of its largest subinterval:

gap⁡(P)=max⁡1≤i≤n (xi−xi−1).\operatorname{gap}(P) = \max_{1 \le i \le n}\,(x_i - x_{i-1}).

It is a number, not an interval. Any sequence of partitions whose gap tends to 00 — even an irregular one built by repeatedly bisecting subintervals — qualifies as Archimedean.

Monotonic functions are integrable. Every monotonic (e.g. increasing) function on a closed interval [a,b][a,b] is bounded (between f(a)f(a) and f(b)f(b)) and integrable. Using a regular partition, the telescoping of the column heights gives the clean estimate

U(f,Pn)−L(f,Pn)=b−an(f(b)−f(a)),U(f,P_n) - L(f,P_n) = \frac{b-a}{n}\bigl(f(b) - f(a)\bigr),

which →0\to 0 as n→∞n\to\infty. Geometrically, the "leftover" rectangles stack into a single box of width b−an\tfrac{b-a}{n} and height f(b)−f(a)f(b)-f(a).

Leibniz notation. Writing ∫abf(x) dx\int_a^b f(x)\,dx records the variable of integration explicitly. Thinking of dxdx as an infinitesimal width and f(x)f(x) as a height, the integral is the limit of ∑f(xi) Δx\sum f(x_i)\,\Delta x: as Δx→0\Delta x \to 0 the deltas become dd's and the sum becomes ∫\int. This makes Leibniz notation natural and flexible (it lets you integrate or differentiate "with respect to" either variable).

Worked Example

Prove every monotonically increasing f:[a,b]→Rf:[a,b]\to\mathbb{R} is integrable. Take regular partitions PnP_n. On each subinterval ff attains its max at the right endpoint (MiM_i) and its min at the left endpoint (mim_i), and every width equals b−an\tfrac{b-a}{n}:

U(f,Pn)−L(f,Pn)=∑i=1nMi b−an−∑i=1nmi b−an=b−an∑i=1n(Mi−mi)=b−an(f(b)−f(a))(the sum telescopes since mi+1=Mi)lim⁡n→∞(U(f,Pn)−L(f,Pn))=lim⁡n→∞(b−a)(f(b)−f(a))n=0.\begin{aligned} U(f,P_n) - L(f,P_n) &= \sum_{i=1}^{n} M_i\,\frac{b-a}{n} - \sum_{i=1}^{n} m_i\,\frac{b-a}{n} \\ &= \frac{b-a}{n}\sum_{i=1}^{n}\bigl(M_i - m_i\bigr) \\ &= \frac{b-a}{n}\bigl(f(b) - f(a)\bigr) \quad\text{(the sum telescopes since } m_{i+1} = M_i\text{)} \\ \lim_{n\to\infty}\bigl(U(f,P_n) - L(f,P_n)\bigr) &= \lim_{n\to\infty}\frac{(b-a)\bigl(f(b)-f(a)\bigr)}{n} = 0. \end{aligned}

By the Archimedes–Riemann theorem, ff is integrable. ■\blacksquare

Compute ∫01x2 dx\int_0^1 x^2\,dx from the definition using the upper sum on a regular partition (a=0, b=1a=0,\ b=1, width 1n\tfrac1n, right endpoints xi=inx_i = \tfrac{i}{n}):

∫01x2 dx=lim⁡n→∞∑i=1nf ⁣(in)1n=lim⁡n→∞∑i=1ni2n2⋅1n=lim⁡n→∞1n3∑i=1ni2=lim⁡n→∞1n3⋅n(n+1)(2n+1)6=lim⁡n→∞2n3+3n2+n6n3=lim⁡n→∞(13+12n+16n2)=13.\begin{aligned} \int_0^1 x^2\,dx &= \lim_{n\to\infty}\sum_{i=1}^{n} f\!\left(\frac{i}{n}\right)\frac{1}{n} = \lim_{n\to\infty}\sum_{i=1}^{n}\frac{i^2}{n^2}\cdot\frac{1}{n} \\ &= \lim_{n\to\infty}\frac{1}{n^3}\sum_{i=1}^{n} i^2 = \lim_{n\to\infty}\frac{1}{n^3}\cdot\frac{n(n+1)(2n+1)}{6} \\ &= \lim_{n\to\infty}\frac{2n^3 + 3n^2 + n}{6n^3} = \lim_{n\to\infty}\left(\frac{1}{3} + \frac{1}{2n} + \frac{1}{6n^2}\right) = \frac{1}{3}. \end{aligned}

Summary