Calculus I · Textbook draft · 21 minute reading

Accumulation and the Definite Integral

Define accumulation through tagged sums, calculate a sum limit exactly, and state what integrability requires.

Before you begin

  • Limits, finite sums, continuity, and elementary area.

Learning objectives

  • Construct tagged Riemann sums with units and signs.
  • Define the definite integral independently of antiderivatives.
  • Evaluate the integral of a square by a finite-sum limit.

A pump’s flow rate is measured in litres per minute. Multiplying a constant rate by time gives transferred volume. For a changing rate, dividing the time interval into short pieces gives a sum of approximate transfers. The definite integral is the limit that makes this accumulation independent of the partition and sample choices, when such a limit exists.

Partitions and tagged sums

A partition a=x0<x1<⋯<xn=ba=x_0<x_1<\cdots<x_n=b divides [a,b][a,b] into widths Δxi=xi−xi−1\Delta x_i=x_i-x_{i-1}. Choose a tag ξi\xi_i in each subinterval. The Riemann sum is

∑i=1nf(ξi)Δxi.\sum_{i=1}^n f(\xi_i)\Delta x_i.

The mesh is max⁡iΔxi\max_i\Delta x_i. A bounded function is Riemann integrable when there is a real number II such that every tagged sum is within any requested tolerance of II once the mesh is sufficiently small. We denote that number by ∫abf(x) dx\int_a^b f(x)\,dx. The definition quantifies over all sufficiently fine partitions and tags; convergence of one favored sequence of sums is not by itself the full definition.

Continuous functions on closed bounded intervals are integrable. Bounded monotone functions are also integrable, even if they have jumps. Not every bounded function is: the function equal to one at rational inputs and zero at irrational inputs on [0,1][0,1] admits tagged sums identically one or identically zero at every mesh, because both types of inputs occur in every subinterval. No common limit exists.

A square integrated from sums

For f(x)=x2f(x)=x^2 on [0,1][0,1], use nn equal pieces and right endpoints i/ni/n. The sum is

Rn=1n∑i=1n(in)2=n(n+1)(2n+1)6n3=13+12n+16n2.R_n=\frac1n\sum_{i=1}^n\left(\frac in\right)^2 =\frac{n(n+1)(2n+1)}{6n^3} =\frac13+\frac1{2n}+\frac1{6n^2}.

We used ∑i2=n(n+1)(2n+1)/6\sum i^2=n(n+1)(2n+1)/6, which can be proved by induction. Thus Rn→1/3R_n\to1/3. The left sum is Ln=1/3−1/(2n)+1/(6n2)L_n=1/3-1/(2n)+1/(6n^2) and tends to the same limit. Because x2x^2 is increasing, every tagged sum for this equal partition lies between these endpoint sums; more generally, continuity supplies integrability for arbitrary fine partitions. Hence ∫01x2 dx=1/3\int_0^1x^2\,dx=1/3.

The sums give a finite-error statement too: Rn−Ln=1/nR_n-L_n=1/n. At n=10n=10, the left and right values are 0.2850.285 and 0.3850.385. Both bracket 1/31/3; neither is the exact integral. A picture of ten rectangles can illustrate the approximation without converting it into equality.

Signed accumulation and units

If ff is negative on part of the interval, its rectangular contributions are negative. Therefore the integral represents signed accumulation. Geometric area between a graph and the axis is ∫ab∣f(x)∣ dx\int_a^b|f(x)|\,dx, not necessarily ∫abf(x) dx\int_a^bf(x)\,dx.

For f(x)=xf(x)=x on [−1,1][-1,1], symmetry gives signed integral zero, although geometric area is one. If ff is velocity, the integral gives displacement; integrating ∣f∣|f| gives distance. If ff is flow in litres per minute and xx is minutes, the integral has units litres. An integral’s units multiply the integrand’s units by those of its input variable.

Properties from sums

Integrals are linear, additive across adjacent intervals, and preserve inequalities for integrable functions. Define ∫baf=−∫abf\int_b^af=-\int_a^bf and ∫aaf=0\int_a^af=0. The reversed orientation is a sign convention consistent with additivity, not a negative geometric interval length in the original partition definition.

If m≤f≤Mm\leq f\leq M on [a,b][a,b], then m(b−a)≤∫abf≤M(b−a)m(b-a)\leq\int_a^bf\leq M(b-a). Also ∣∫f∣≤∫∣f∣|\int f|\leq\int|f|. These bounds can detect an impossible answer before an exact calculation is available.

Exercises

  1. Write the right-endpoint sum for f(x)=3xf(x)=3x on [0,2][0,2] and calculate its limit.
  2. Compute left and right sums for x2x^2 on [0,1][0,1] with n=4n=4.
  3. If 2≤f(x)≤52\leq f(x)\leq5 on [1,4][1,4], bound its integral.
  4. Explain why an integral of a velocity can be zero while distance travelled is positive.
  5. Show that changing a bounded integrable function at one point does not alter its integral.
  6. Why does the rational-indicator example not become integrable when a single fine regular grid happens to choose only irrational tags?
Worked solutions
  1. The width is 2/n2/n, tag 2i/n2i/n, giving (12/n2)∑i=6(n+1)/n→6(12/n^2)\sum i=6(n+1)/n\to6.
  2. L4=0.21875L_4=0.21875 and R4=0.46875R_4=0.46875, using the displayed formulas.
  3. Between 66 and 1515.
  4. Opposite-direction displacements can cancel. Distance adds their magnitudes.
  5. If the changed value differs by at most BB, only subintervals touching that point can be affected. Their total contribution difference is bounded by 2B2B times the mesh, tending to zero. Interior tags usually affect one piece; allowing two handles shared endpoints.
  6. Integrability requires all sufficiently fine tagged sums to converge to the same number. Rational tags still give one, while irrational tags give zero.