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Riemann Integration | Mathematics

Let f:[a,b]Rf : [a,b] \to \mathbb{R} be bounded. A partition of [a,b][a,b] is a finite set P={x0,x1,,xn}P = \{x_0, x_1, \ldots, x_n\} with a=x0<x1<<xn=ba = x_0 \lt x_1 \lt \cdots \lt x_n = b.

The upper sum and lower sum of ff with respect to PP are:

U(f,P)=i=1nMiΔxi,L(f,P)=i=1nmiΔxiU(f, P) = \sum_{i=1}^{n} M_i \Delta x_i, \quad L(f, P) = \sum_{i=1}^{n} m_i \Delta x_i

Where Mi=sup{f(x):x[xi1,xi]}M_i = \sup\{f(x) : x \in [x_{i-1}, x_i]\}, mi=inf{f(x):x[xi1,xi]}m_i = \inf\{f(x) : x \in [x_{i-1}, x_i]\} And Δxi=xixi1\Delta x_i = x_i - x_{i-1}.

The mesh of PP is P=max1inΔxi\|P\| = \max_{1 \leq i \leq n} \Delta x_i.

Definition. ff is Riemann integrable on [a,b][a,b] if the upper and lower integrals are equal:

abf(x)dx=abf(x)dx\overline{\int_a^b} f(x)\, dx = \underline{\int_a^b} f(x)\, dx

Where abf=inf{U(f,P):P is a partition}\overline{\int_a^b} f = \inf\{U(f,P) : P \mathrm{\ is\ a\ partition}\} and abf=sup{L(f,P):P is a partition}\underline{\int_a^b} f = \sup\{L(f,P) : P \mathrm{\ is\ a\ partition}\}.

The common value is denoted abf(x)dx\int_a^b f(x)\, dx.

Theorem 6.1 (Riemann Integrability Criterion). A bounded function f:[a,b]Rf : [a,b] \to \mathbb{R} is Riemann integrable if and only if for every ε>0\varepsilon > 0There exists a partition PP such that

U(f,P)L(f,P)<εU(f,P) - L(f,P) \lt \varepsilon

Theorem 6.2. Every continuous function on [a,b][a,b] is Riemann integrable.

Proof. Let ff be continuous on [a,b][a,b]. By the Heine-Cantor theorem, ff is uniformly continuous. Given ε>0\varepsilon > 0Choose δ>0\delta > 0 such that xy<δ|x - y| \lt \delta implies f(x)f(y)<ε/(ba)|f(x) - f(y)| \lt \varepsilon/(b-a).

Let PP be any partition with P<δ\|P\| \lt \delta. On each subinterval [xi1,xi][x_{i-1}, x_i]By the Extreme Value Theorem, ff attains its maximum MiM_i and minimum mim_i. By uniform continuity: Mimi<ε/(ba)M_i - m_i \lt \varepsilon/(b-a). Therefore:

U(f,P)L(f,P)=i=1n(Mimi)Δxi<εbai=1nΔxi=εU(f,P) - L(f,P) = \sum_{i=1}^{n}(M_i - m_i)\Delta x_i \lt \frac{\varepsilon}{b-a} \sum_{i=1}^{n} \Delta x_i = \varepsilon

By the Riemann integrability criterion, ff is integrable. \blacksquare

Theorem 6.3. Every monotone function on [a,b][a,b] is Riemann integrable.

Proof. Assume ff is increasing (the decreasing case is analogous). Given ε>0\varepsilon > 0Let PnP_n be the uniform partition with nn subintervals of length (ba)/n(b-a)/n. On [xi1,xi][x_{i-1}, x_i]: Mi=f(xi)M_i = f(x_i) and mi=f(xi1)m_i = f(x_{i-1}). Then:

U(f,Pn)L(f,Pn)=i=1n[f(xi)f(xi1)]ban=[f(b)f(a)]banU(f, P_n) - L(f, P_n) = \sum_{i=1}^{n} [f(x_i) - f(x_{i-1})] \cdot \frac{b-a}{n} = [f(b) - f(a)] \cdot \frac{b-a}{n}

Choose nn large enough that [f(b)f(a)](ba)/n<ε[f(b) - f(a)](b-a)/n \lt \varepsilon. \blacksquare

Theorem 6.4. A bounded function with finitely many discontinuities on [a,b][a,b] is Riemann integrable.

Proof (sketch). Let ff have discontinuities at d1,,dm[a,b]d_1, \ldots, d_m \in [a,b]. Given ε>0\varepsilon > 0 Enclose each djd_j in a small interval IjI_j of total length ε/(2M)\varepsilon/(2M)Where M=sup[a,b]fM = \sup_{[a,b]} |f|. On the remaining set (a finite union of closed intervals), ff is continuous, Hence uniformly continuous. Choose a partition fine enough that the oscillation of ff on each Subinterval outside the IjI_j is less than ε/(2(ba))\varepsilon/(2(b-a)). Then:

U(f,P)L(f,P)ε2(ba)(ba)+2Mε2M=εU(f, P) - L(f, P) \leq \frac{\varepsilon}{2(b-a)} \cdot (b - a) + 2M \cdot \frac{\varepsilon}{2M} = \varepsilon

\blacksquare

Proposition 6.4a. The set of Riemann integrable functions on [a,b][a,b] forms a vector space, and If ff and gg are integrable, then so are f|f|, f2f^2 And max(f,g)\max(f, g).

Theorem 6.4b (Lebesgue”s Criterion for Riemann Integrability). A bounded function f:[a,b]Rf : [a,b] \to \mathbb{R} Is Riemann integrable if and only if the set of its discontinuities has (Lebesgue) measure zero.

Remark. A set has measure zero if it can be covered by countably many intervals of arbitrarily Small total length. In particular, every countable set has measure zero. This means:

  • Every continuous function is integrable (empty set of discontinuities).
  • Every function with countably many discontinuities is integrable (Theorem 6.4 is a special case).
  • The Dirichlet function f(x)=1f(x) = 1 for xQx \in \mathbb{Q} and f(x)=0f(x) = 0 for xQx \notin \mathbb{Q} is discontinuous everywhere (set of discontinuities = [a,b][a,b]Measure >0> 0), hence not integrable.
  • Thomae’s function f(x)=1/qf(x) = 1/q if x=p/qx = p/q in lowest terms, and f(x)=0f(x) = 0 if xx is irrational, is continuous at every irrational and discontinuous at every rational. Since Q\mathbb{Q} is countable (measure zero), Thomae’s function is Riemann integrable, with 01f=0\int_0^1 f = 0.

Theorem 6.5 (Linearity). If ff and gg are integrable on [a,b][a,b] and α,βR\alpha, \beta \in \mathbb{R}:

ab(αf+βg)=αabf+βabg\int_a^b (\alpha f + \beta g) = \alpha \int_a^b f + \beta \int_a^b g

Theorem 6.6 (Monotonicity). If f(x)g(x)f(x) \leq g(x) for all x[a,b]x \in [a,b] Then abfabg\int_a^b f \leq \int_a^b g.

Theorem 6.7 (Triangle Inequality). abfabf\left|\int_a^b f\right| \leq \int_a^b |f|.

Theorem 6.8 (FTC Part 1). If ff is continuous on [a,b][a,b] Then the function

F(x)=axf(t)dtF(x) = \int_a^x f(t)\, dt

Is differentiable on (a,b)(a,b) and F(x)=f(x)F'(x) = f(x).

Proof. Let h>0h > 0 (the case h<0h \lt 0 is similar). By the Mean Value Theorem for Integrals (which follows from the EVT), there exists ξ[x,x+h]\xi \in [x, x+h] such that

F(x+h)F(x)h=1hxx+hf(t)dt=f(ξ)\frac{F(x+h) - F(x)}{h} = \frac{1}{h}\int_x^{x+h} f(t)\, dt = f(\xi)

As h0+h \to 0^+We have ξx+\xi \to x^+ (since ξ[x,x+h]\xi \in [x, x+h]). By continuity of ff f(ξ)f(x)f(\xi) \to f(x). Hence F+(x)=f(x)F'_+(x) = f(x). A similar argument gives F(x)=f(x)F'_-(x) = f(x). \blacksquare

Theorem 6.9 (FTC Part 2). If FF is differentiable on [a,b][a,b] with F=fF' = f (and ff is integrable), Then

abf(x)dx=F(b)F(a)\int_a^b f(x)\, dx = F(b) - F(a)

Proof. Let P={x0,,xn}P = \{x_0, \ldots, x_n\} be any partition of [a,b][a,b]. By the Mean Value Theorem, For each ii there exists ξi[xi1,xi]\xi_i \in [x_{i-1}, x_i] with F(xi)F(xi1)=f(ξi)ΔxiF(x_i) - F(x_{i-1}) = f(\xi_i)\Delta x_i. Summing:

F(b)F(a)=i=1n[F(xi)F(xi1)]=i=1nf(ξi)ΔxiF(b) - F(a) = \sum_{i=1}^{n} [F(x_i) - F(x_{i-1})] = \sum_{i=1}^{n} f(\xi_i) \Delta x_i

The right-hand side is a Riemann sum for abf\int_a^b f. As P0\|P\| \to 0This converges to the Integral. Hence F(b)F(a)=abf(x)dxF(b) - F(a) = \int_a^b f(x)\, dx. \blacksquare

Problem. Compute 01x2dx\int_0^1 x^2\, dx from the definition.

Solution. Let Pn={0,1/n,2/n,,1}P_n = \{0, 1/n, 2/n, \ldots, 1\}. On [xi1,xi]=[(i1)/n,i/n][x_{i-1}, x_i] = [(i-1)/n, i/n], f(x)=x2f(x) = x^2 Has Mi=(i/n)2M_i = (i/n)^2 and mi=((i1)/n)2m_i = ((i-1)/n)^2.

U(f,Pn)=i=1ni2n21n=1n3i=1ni2=1n3n(n+1)(2n+1)6U(f, P_n) = \sum_{i=1}^{n} \frac{i^2}{n^2} \cdot \frac{1}{n} = \frac{1}{n^3} \sum_{i=1}^{n} i^2 = \frac{1}{n^3} \cdot \frac{n(n+1)(2n+1)}{6}

As nn \to \infty: limnU(f,Pn)=limn(n+1)(2n+1)6n2=26=13\lim_{n \to \infty} U(f, P_n) = \lim_{n \to \infty} \frac{(n+1)(2n+1)}{6n^2} = \frac{2}{6} = \frac{1}{3}.

Similarly, L(f,Pn)1/3L(f, P_n) \to 1/3. So 01x2dx=1/3\int_0^1 x^2\, dx = 1/3. \blacksquare

Worked Example: Compute $\int_0^1 \sqrt{x}\, dx$ from the definition

Solution. Let Pn={0,1/n,2/n,,1}P_n = \{0, 1/n, 2/n, \ldots, 1\}. On [(i1)/n,i/n][(i-1)/n, i/n], f(x)=xf(x) = \sqrt{x} has Mi=i/nM_i = \sqrt{i/n} and mi=(i1)/nm_i = \sqrt{(i-1)/n}.

U(f,Pn)=i=1nin1n=1n3/2i=1niU(f, P_n) = \sum_{i=1}^{n} \sqrt{\frac{i}{n}} \cdot \frac{1}{n} = \frac{1}{n^{3/2}} \sum_{i=1}^{n} \sqrt{i}

Using i=1ni=23n3/2+O(n1/2)\sum_{i=1}^{n} \sqrt{i} = \frac{2}{3} n^{3/2} + O(n^{1/2}) (obtained from comparing with 0nxdx\int_0^n \sqrt{x}\, dx):

limnU(f,Pn)=limn1n3/223n3/2=23\lim_{n \to \infty} U(f, P_n) = \lim_{n \to \infty} \frac{1}{n^{3/2}} \cdot \frac{2}{3}n^{3/2} = \frac{2}{3}

Similarly L(f,Pn)2/3L(f, P_n) \to 2/3Confirming 01xdx=2/3\int_0^1 \sqrt{x}\, dx = 2/3. \blacksquare

Definition. An improper integral is a Riemann integral where either the interval of integration Is unbounded or the integrand is unbounded.

Type I (Infinite Intervals). If ff is Riemann integrable on [a,b][a, b] for every b>ab > aDefine:

af(x)dx=limbabf(x)dx\int_a^{\infty} f(x)\, dx = \lim_{b \to \infty} \int_a^b f(x)\, dx

The integral converges if this limit exists as a finite number; otherwise it diverges.

Type II (Unbounded Integrands). If ff is unbounded near aa but integrable on [c,b][c, b] for every c(a,b]c \in (a, b]:

abf(x)dx=limca+cbf(x)dx\int_a^b f(x)\, dx = \lim_{c \to a^+} \int_c^b f(x)\, dx

Theorem 6.10 (Comparison Test for Improper Integrals). If 0f(x)g(x)0 \leq f(x) \leq g(x) for xax \geq a:

  • If ag\int_a^{\infty} g converges, then af\int_a^{\infty} f converges.
  • If af\int_a^{\infty} f diverges, then ag\int_a^{\infty} g diverges.

Theorem 6.11 (Absolute Convergence). If af(x)dx\int_a^{\infty} |f(x)|\, dx converges, then af(x)dx\int_a^{\infty} f(x)\, dx converges.

Theorem 6.12 (pp-Test for Improper Integrals).

  • Type I: 11xpdx\int_1^{\infty} \frac{1}{x^p}\, dx converges if and only if p>1p > 1.
  • Type II: 011xpdx\int_0^1 \frac{1}{x^p}\, dx converges if and only if p<1p < 1.

Proof. For Type I with p1p \neq 1:

1xpdx=limb[x1p1p]1b=limbb1p11p\int_1^{\infty} x^{-p}\, dx = \lim_{b \to \infty} \left[\frac{x^{1-p}}{1-p}\right]_1^b = \lim_{b \to \infty} \frac{b^{1-p} - 1}{1-p}

This converges when 1p<01 - p < 0I.e., p>1p > 1. For p=1p = 1: 11/xdx=limblnb=\int_1^{\infty} 1/x\, dx = \lim_{b \to \infty} \ln b = \infty.

For Type II: 01xpdx=limc0+1c1p1p\int_0^1 x^{-p}\, dx = \lim_{c \to 0^+} \frac{1 - c^{1-p}}{1-p}. This converges when 1p>01 - p > 0I.e., p<1p < 1. \blacksquare

Remark. The pp-test for Type I integrals mirrors the pp-series test: 1/np\sum 1/n^p converges Iff p>1p > 1. This is not a coincidence --- the integral test establishes the connection.

Worked Example: Evaluate $\int_0^{\infty} e^{-x}\, dx$

Solution. This is a Type I improper integral:

0exdx=limb0bexdx=limb[ex]0b=limb(eb+1)=1\int_0^{\infty} e^{-x}\, dx = \lim_{b \to \infty} \int_0^b e^{-x}\, dx = \lim_{b \to \infty} \left[-e^{-x}\right]_0^b = \lim_{b \to \infty} (-e^{-b} + 1) = 1

So the integral converges to 11. \blacksquare

Worked Example: Does $\int_1^{\infty} \frac{\sin x}{x}\, dx$ converge?

Solution. The integral 1sinxxdx\int_1^{\infty} \left|\frac{\sin x}{x}\right|\, dx diverges (compare with 1sinxxdxk=1kπ(k+1)πsinxxdxk=12(k+1)π\int_1^{\infty} \frac{|\sin x|}{x}\, dx \geq \sum_{k=1}^{\infty} \int_{k\pi}^{(k+1)\pi} \frac{|\sin x|}{x}\, dx \geq \sum_{k=1}^{\infty} \frac{2}{(k+1)\pi}, which diverges by comparison with the harmonic series).

However, 1sinxxdx\int_1^{\infty} \frac{\sin x}{x}\, dx converges by Dirichlet’s test for integrals. Let F(b)=1bsinxdx=cos1cosbF(b) = \int_1^b \sin x\, dx = \cos 1 - \cos bWhich is bounded by cos1cosb2|\cos 1 - \cos b| \leq 2. Since 1/x1/x decreases to 00By integration by parts:

1bsinxxdx=cosxx1b1bcosxx2dx\int_1^b \frac{\sin x}{x}\, dx = \frac{-\cos x}{x}\bigg|_1^b - \int_1^b \frac{\cos x}{x^2}\, dx

As bb \to \inftyThe boundary term cosb/b0\cos b / b \to 0 and 1cosxx2dx11x2dx=1\int_1^{\infty} \frac{|\cos x|}{x^2}\, dx \leq \int_1^{\infty} \frac{1}{x^2}\, dx = 1, so the improper integral converges (conditionally). \blacksquare

Worked Example: Evaluate $\int_0^1 \frac{1}{\sqrt{x}}\, dx$ (Type II improper integral)

Solution. The integrand f(x)=1/xf(x) = 1/\sqrt{x} is unbounded as x0+x \to 0^+. Compute:

011xdx=limc0+c1x1/2dx=limc0+[2x]c1=limc0+(22c)=2\int_0^1 \frac{1}{\sqrt{x}}\, dx = \lim_{c \to 0^+} \int_c^1 x^{-1/2}\, dx = \lim_{c \to 0^+} \left[2\sqrt{x}\right]_c^1 = \lim_{c \to 0^+} (2 - 2\sqrt{c}) = 2

The improper integral converges to 22. Note that 01xpdx\int_0^1 x^{-p}\, dx converges for p<1p \lt 1 and Diverges for p1p \geq 1. \blacksquare

Worked Example: Determine convergence of $\int_1^{\infty} \frac{1}{x^p}\, dx$ for various $p$

Solution. By the pp-test (Theorem 6.12): 1xpdx\int_1^{\infty} x^{-p}\, dx converges iff p>1p > 1.

Specifically:

  • p=2p = 2: 11/x2dx=limb[1/x]1b=0(1)=1\int_1^{\infty} 1/x^2\, dx = \lim_{b \to \infty} [-1/x]_1^b = 0 - (-1) = 1. Converges.
  • p=1p = 1: 11/xdx=limblnb=\int_1^{\infty} 1/x\, dx = \lim_{b \to \infty} \ln b = \infty. Diverges.
  • p=1/2p = 1/2: 11/xdx=limb[2x]1b=\int_1^{\infty} 1/\sqrt{x}\, dx = \lim_{b \to \infty} [2\sqrt{x}]_1^b = \infty. Diverges.

This mirrors the pp-series test: 1/np\sum 1/n^p converges iff p>1p > 1. \blacksquare

Worked Example: Evaluate $\int_0^{\infty} x e^{-x}\, dx$

Solution. This integral requires both a Type I and Type II limit:

0xexdx=lima0+limbabxexdx\int_0^{\infty} x e^{-x}\, dx = \lim_{a \to 0^+} \lim_{b \to \infty} \int_a^b x e^{-x}\, dx

Integrate by parts with u=xu = x, dv=exdxdv = e^{-x}\, dx So du=dxdu = dx, v=exv = -e^{-x}:

xexdx=xex+exdx=xexex=(x+1)ex\int x e^{-x}\, dx = -xe^{-x} + \int e^{-x}\, dx = -xe^{-x} - e^{-x} = -(x+1)e^{-x}

Evaluating: limb[(b+1)eb]lima0+[(a+1)ea]=0(1)=1\lim_{b \to \infty} [-(b+1)e^{-b}] - \lim_{a \to 0^+} [-(a+1)e^{-a}] = 0 - (-1) = 1.

So 0xexdx=1\int_0^{\infty} x e^{-x}\, dx = 1. This equals Γ(2)=1!=1\Gamma(2) = 1! = 1. \blacksquare

Mistake 1: Confusing Riemann integrability with Lebesgue integrability Every Riemann integrable function is Lebesgue integrable, but not vice versa. The Dirichlet function is not Riemann integrable but is Lebesgue integrable (with integral zero). The Riemann integral requires the set of discontinuities to have measure zero, while the Lebesgue integral handles a much broader class of functions.

Mistake 2: Interchanging limits and integrals without justification Swapping lim\lim and \int requires a convergence theorem such as the dominated convergence theorem or the monotone convergence theorem. Pointwise convergence alone is insufficient: the sequence fn=nχ(0,1/n)f_n = n\chi_{(0, 1/n)} converges pointwise to 00 on [0,1][0, 1], yet 01fn=1\int_0^1 f_n = 1 for all nn. Always verify the hypotheses of a convergence theorem before interchanging limits and integrals.

Mistake 3: Applying the Fundamental Theorem of Calculus to discontinuous integrands The FTC Part 1 requires ff to be continuous. If ff has a jump discontinuity, the integral function F(x)=axf(t)dtF(x) = \int_a^x f(t)\,dt is continuous but not differentiable at the discontinuity. The FTC Part 2 requires F=fF' = f everywhere on [a,b][a, b], which fails if ff is discontinuous. Check continuity before applying the FTC.

The Riemann integral answers the question: how do we add up infinitely many infinitely thin slices? Consider the area under a curve f(x) from a to b. The Riemann sum approximates this by dividing the interval into subintervals and summing f(x) times the width of each subinterval — a collection of rectangles whose total area approaches the true area as the partition becomes finer. This is the same logic as computing distance by summing velocity over time, or charge by summing current over time: the integral accumulates a quantity that varies continuously.

The Fundamental Theorem of Calculus reveals the deep connection between accumulation (integration) and rate of change (differentiation). If F(x) represents the accumulated area from a to x, then F’(x) = f(x): the rate at which area accumulates is exactly the height of the curve. Conversely, integrating a rate function recovers the total change. This duality is why the FTC is the most important theorem in calculus: it converts the hard problem of computing areas into the easy problem of finding antiderivatives. The improper integral extends this to infinite intervals or unbounded functions by taking limits, but the core intuition — accumulation of slices — remains the same.