5.2 The Definite Integral

The definite integral as the limit of Riemann sums, its notation and the meaning of each part, net signed area against total area, which functions are integrable, the properties inherited from sums, and the average value of a function.

Subject: Calculus I · 65 slides · symbolic lesson

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What this lesson covers

The lesson, slide by slide

1. Section 5.2 The Definite Integral

Title

Calculus I · Chapter 5 — Integration

The Definite Integral

2. By the end of this lesson you can

Objectives

Five outcomes. The first is a definition, and the rest are what can be done with it before any antiderivative appears.

OpenStax Calculus Volume 1, §5.2 The Definite Integral §5.2, pp. 456-471 — the section these objectives are drawn from

3. What you already have

Warm-up

Section 5.1 built rectangle approximations and showed their limit exists and does not depend on the sample points chosen.

Discussion prompt

That limit deserves a name and a symbol. What should the symbol look like?

Hint: It is replacing a sum of heights times widths.

Answer:

The limit replaces a sigma with an elongated S — the same letter, stretched — and the width, which shrank to nothing, becomes the dx. The heights stay as the function.

\[ \lim_{n\to\infty}\sum_{i=1}^{n}f(x_{i}^{*})\,\Delta x \;\longrightarrow\; \int_{a}^{b}f(x)\,dx \]

Every symbol in the new notation traces back to one in the old. Beyond notation, this section establishes what can be done with these objects — splitting them, comparing them, bounding them — all before Section 5.3 shows how to compute one quickly.

4. The limit, named and given rules

Concept

The definite integral of a function over an interval is the limit of its Riemann sums. It represents net signed area, counting regions below the axis as negative, and it obeys a set of properties inherited from sums.

definite integral — The limit of Riemann sums for a function on a closed interval, when that limit exists independently of the sample points. It is a number, not a family of functions.

\[ \int_{a}^{b}f(x)\,dx = \lim_{n\to\infty}\sum_{i=1}^{n}f(x_{i}^{*})\,\Delta x \]

The word definite distinguishes this from Section 4.10's indefinite integral. That one produced a family of functions; this produces a single number, and the two are connected by the theorem of Section 5.3.

Figure (svg): Definite integral notation, with each part named and the Riemann sum it came from

The symbol was chosen to look like the sum it replaces, and the dx is the width that shrank to nothing.

OpenStax Calculus Volume 1, §5.2 The Definite Integral §5.2, pp. 462-470

5. Definition and notation

Section

Section 1

6. Every symbol traces back to the sum

Concept

The integral sign is a stretched sigma, the integrand is the height, the differential is the vanished width, and the numbers on the sign are the interval's ends.

limits of integration — The numbers at the bottom and top of the integral sign, naming the interval's left and right ends. They are not limits in the Chapter 2 sense, despite the name.

\[ \int_{a}^{b}f(x)\,dx: \; a \text{ lower}, \; b \text{ upper}, \; f \text{ integrand}, \; x \text{ variable} \]

The variable of integration is a placeholder like a sum's index: the integral of f of x with respect to x and the integral of f of t with respect to t over the same interval are the same number.

Figure (svg): Definite integral notation, with each part named and the Riemann sum it came from

The symbol was chosen to look like the sum it replaces, and the dx is the width that shrank to nothing.

OpenStax Calculus Volume 1, §5.2 The Definite Integral §5.2, pp. 462-470 — definition and notation

7. From the sum to the symbol

Picture it

Each part named.

Figure (svg): Definite integral notation, with each part named and the Riemann sum it came from

The symbol was chosen to look like the sum it replaces, and the dx is the width that shrank to nothing.

Notice the differential's role has shifted. In Section 4.10 it named the variable; here it does that and also records where the width went, which is why it must not be omitted.

8. Worked example: expressing a limit as an integral

Worked example

Example 5.10. Reading a Riemann sum backwards.

\[ \text{Express } \lim_{n\to\infty}\sum_{i=1}^{n}\left(2+\frac{3i}{n}\right)^{2}\frac{3}{n} \text{ as an integral.} \]

Identify the width

Why: The factor not depending on the function.

\[ \frac{3}{n},\text{ so } b - a = 3 \]

Identify the sample points

Why: The expression inside.

\[ x _{i} = 2 + 3 i / n \]

Read off the left end

Why: At i equal to 0.

\[ a = 2 \]

Read off the right end

Why: Left end plus the total width.

\[ b = 5 \]

Identify the function

Why: What is applied to the sample point.

\[ f(x) = x ^{2} \]

Figure (svg): Definite integral notation, with each part named and the Riemann sum it came from

The symbol was chosen to look like the sum it replaces, and the dx is the width that shrank to nothing.

\[ \int_{2}^{5}x^{2}\,dx \]

Verify: check the width against the interval

Why: The interval from 2 to 5 has length 3, and dividing it into n pieces gives width 3 over n — which is exactly the factor in the sum. The sample points run from 2 plus 3 over n up to 5, confirming right endpoints on that interval. Reading a Riemann sum backwards like this is the skill Section 5.3 will need in reverse, and the width factor is always the giveaway.

OpenStax Calculus Volume 1, §5.2 The Definite Integral §5.2, pp. 466-467

9. Read off the interval

Fill the middle

A Riemann sum whose width factor is three over n.

Fill in the blanks

\Delta x = \frac3___ \;\Longrightarrow\; b-a = ___

Why: The width is the interval length over n, so the length is 3. Combined with the sample points starting at 2, the interval is from 2 to 5.

10. Worked example: the variable is a placeholder

Worked example

Checkpoint 5.10. Renaming changes nothing.

\[ \text{Are } \int_{0}^{2}x^{2}dx \text{ and } \int_{0}^{2}t^{2}dt \text{ the same?} \]

Write the Riemann sum for the first

Why: Sample points and width.

Write it for the second

Why: The same construction.

Compare

Why: Identical numbers throughout.

Take limits

Why: Identical limits.

Conclude

Why: The letter is a placeholder.

Figure (svg): The solution to Worked example the variable is a placeholder shown as a ladder of expressions, one row per legal move

The whole solution at once: each drop is one legal move.

\[ \int_{0}^{2}x^{2}dx = \int_{0}^{2}t^{2}dt = \tfrac83 \]

Verify: contrast this with the indefinite integral

Why: For an INDEFINITE integral the letter does matter in the answer: Section 4.10 showed the antiderivative of t cubed with respect to t is t to the fourth over 4, in the variable t. But a definite integral is a number, and a number carries no variable — so the letter vanishes with the limit. This is why the variable of integration is called a dummy variable, exactly like a sum's index.

OpenStax Calculus Volume 1, §5.2 The Definite Integral §5.2, pp. 467-468

11. Trap: the variable of integration appearing in the answer

Trap

The trap

\[ \int_{0}^{2}x^{2}\,dx = \frac{x^{3}}{3}\bigg|_{0}^{2} = \frac{x^{3}}{3} \]

Leave the variable in the final answer

Why: The student stops before substituting.

A definite integral is a number. An answer containing x is not a number and cannot be one.

The fix

\[ = \frac{8}{3}-0 = \frac{8}{3} \]

Substitute both limits and subtract, leaving a number

Why: The variable disappears with the evaluation.

A quick check on any definite integral: if the answer contains the variable of integration, something has been left undone. That single test catches this error every time.

12. Symbol to its origin

Matching

Each part came from the Riemann sum.

Match the pairs

  • l1. the elongated S
  • l2. the integrand
  • l3. the dx
  • l4. the two numbers on the sign
  • r1. the sigma
  • r2. the rectangle heights
  • r3. the width, shrunk to nothing
  • r4. the interval's ends

Why: The notation was designed so that every piece of the sum survives visibly in the limit. Leibniz chose it deliberately, and it is why the symbol is so easy to read once the sum behind it is understood.

13. One of these claims is false

Two truths and a lie

All three are about notation.

Eliminate the wrong options

Two of these are true. Knock those out and keep the false one.

  • A. The variable of integration can be renamed freely
  • C. A definite integral is a number, not a function
  • B. The limits of integration are limits in the Chapter 2 sense

Survives elimination: B

Why: The survivor is the false one. The word limit is doing two different jobs: the limits of integration are just the interval's endpoints, while the limit in the definition is the Chapter 2 kind, taken as n grows. The clash of terminology is unfortunate but standard.

14. Why does the letter vanish?

Prediction

Commit before reasoning.

Predict first

Why can the variable of integration be renamed without changing a definite integral?

  • It cannot
  • Because the result is a number, and a number contains no variable
  • Because x and t are the same
  • By convention

Correct: Because the result is a number.

\[ \int_{0}^{2}x^{2}dx = \tfrac83, \quad \int x^{2}dx = \tfrac{x^{3}}{3}+C \]

Why: The variable exists only inside the construction — it labels the sample points that get summed — and both the sum and its limit produce a single number with no variable left in it. Contrast the indefinite integral, which produces a function and where the letter genuinely survives into the answer. That difference is the clearest way to keep the two objects apart.

15. Net signed area

Section

Section 2

16. Below the axis counts negative

Concept

Where the function is negative, its rectangles have negative height, so those contributions subtract. The integral therefore gives net signed area, which can be zero or negative even for a region of substantial size.

net signed area — The area above the axis minus the area below it. It is what the integral computes, and it differs from total area whenever the function changes sign.

\[ \int_{0}^{2\pi}\sin x\,dx = 0 \]

To get total area instead, integrate the absolute value — which in practice means splitting at the zeros and negating the pieces below the axis before adding.

Figure (svg): Net signed area: regions below the axis counted negative

This is the single most important distinction in the section: the integral gives net signed area, which is not the same as total area.

OpenStax Calculus Volume 1, §5.2 The Definite Integral §5.2, pp. 468-474 — net signed area

17. Two halves that cancel

Picture it

A full period of the sine.

Figure (svg): Net signed area: regions below the axis counted negative

This is the single most important distinction in the section: the integral gives net signed area, which is not the same as total area.

The integral is exactly zero although the region has area 4. Nothing has gone wrong: the integral was never a measure of total area, and asking it for one is asking the wrong question.

18. Worked example: signed against total area

Worked example

Example 5.12. The same region, two questions.

\[ \text{For } f(x)=\sin x \text{ on } [0,2\pi], \text{ find the integral and the total area.} \]

Find where the function changes sign

Why: The zeros inside the interval.

Note the first half is above the axis

Why: Positive contribution.

\[ \text{area } 2 \]

Note the second half is below

Why: Negative contribution.

\[ -2 \]

Add for the integral

Why: The signed total.

\[ 0 \]

Add magnitudes for total area

Why: Negating the lower piece.

\[ 2 + 2 = 4 \]

Figure (svg): Net signed area: regions below the axis counted negative

This is the single most important distinction in the section: the integral gives net signed area, which is not the same as total area.

\[ \int_{0}^{2\pi}\sin x\,dx = 0, \qquad \text{total area} = 4 \]

Verify: confirm the cancellation is exact and say why

Why: The sine's second half is the exact reflection of its first through the point at pi, so the two regions are congruent and the cancellation is exact rather than approximate. Note that the integral being zero says something true and useful — over a full period the sine's net contribution vanishes, which is why alternating currents deliver no net charge — but it is a different fact from the region's size.

OpenStax Calculus Volume 1, §5.2 The Definite Integral §5.2, pp. 470-471

19. Signed or total?

Sorting

What is the question actually asking?

Sort into buckets

Sort each question by which quantity answers it.

Net signed area
evaluate the integral of sin x over a full period; the net displacement of a particle from its velocity; the net charge delivered by an alternating current
Total area
find the total area between sin x and the axis there; the total distance the particle travelled
signed
Opposite contributions genuinely cancel: going backwards undoes going forwards, and current in one direction undoes current in the other.
total
Contributions accumulate regardless of sign: distance travelled and geometric area both count every part positively.

The displacement-against-distance pair is the clearest case. A particle returning to its start has zero displacement and a substantial distance travelled, and the same integral answers only the first.

20. Worked example: computing total area

Worked example

Checkpoint 5.12. Split at the zeros.

\[ \text{Find the total area between } f(x)=x-1 \text{ and the axis on } [0,3]. \]

Find the zero

Why: Set the function to zero.

\[ x = 1 \]

Split the interval there

Why: Two pieces.

\[ [0, 1]\text{ and } [1, 3] \]

Compute the first piece

Why: A triangle below the axis.

\[ \text{signed value } -\frac{1}{2} \]

Compute the second

Why: A triangle above.

\[ \text{signed value } 2 \]

Add magnitudes

Why: Negate the first.

\[ \frac{1}{2} + 2 = \frac{5}{2} \]

Figure (svg): The solution to Worked example computing total area shown as a ladder of expressions, one row per legal move

The whole solution at once: each drop is one legal move.

\[ \text{total} = \tfrac52, \qquad \int_{0}^{3}(x-1)dx = \tfrac32 \]

Verify: check both against the geometry

Why: The two triangles have bases 1 and 2 and heights 1 and 2, giving areas one half and 2 — matching. The integral, at three halves, is the difference rather than the sum, which is exactly two times one half less than the total. Splitting at the zeros is the essential move: attempting the total area in one integral gives the signed value instead, and the difference is invisible in the arithmetic.

OpenStax Calculus Volume 1, §5.2 The Definite Integral §5.2, pp. 471-473

21. Find the error: total area computed as one integral

Error analysis

A student is asked for the total area between a curve and the axis.

Annotate

On: \( \text{total area} = \int_{0}^{2\pi}\sin x\,dx = 0 \)

  • The integral is computed correctly: it is indeed zero.
  • But the question asked for AREA, and an area cannot be zero for a non-empty region.
  • The integral gave net signed area, in which the two halves cancelled.
  • Splitting at pi and adding magnitudes gives the correct total of 4.

The answer of zero should itself have been the warning. An area is never negative and is zero only for an empty region, so any signed-looking answer to an area question means the sign changes were not handled.

22. Compute the total area

Fill the middle

A sine over a full period, split at its interior zero.

Fill in the blanks

\text4 = 2 + |___| = ___

Why: The two halves each have area 2, and the total counts both positively. The integral, which subtracts them, gives zero — a different and equally correct answer to a different question.

23. Order the total-area computation

Ranking

A function that crosses the axis.

Put in order

  1. Find where the function is zero inside the interval
  2. Split the interval at those points
  3. Integrate over each piece separately
  4. Take the magnitude of each result
  5. Add the magnitudes

Why: Step d is what distinguishes this from the signed computation, and step a is what makes it possible. Skipping the split and taking one magnitude at the end gives the magnitude of the signed value, which is not the total area.

24. Why zero, not four?

Prediction

Commit before reasoning.

Predict first

The integral of the sine over a full period is zero. Has something gone wrong?

  • Yes: the area should be 4
  • No: the integral gives net signed area, and the two halves cancel exactly
  • Yes: the sine is not integrable there
  • No: the area really is zero

Correct: No: the integral gives signed area and the halves cancel.

\[ \int_{0}^{2\pi}\sin x\,dx = 0 \quad \text{but} \quad \int_{0}^{2\pi}|\sin x|\,dx = 4 \]

Why: The region genuinely has area 4, and the integral genuinely is zero — both are correct answers to different questions. The integral counts area below the axis negatively, which is exactly what makes it the right tool for displacement, net charge and net change, where opposite contributions really do cancel. For geometric area the integrand must be split at its zeros first.

25. Which functions are integrable

Section

Section 3

26. Continuity is enough, but not required

Concept

Every continuous function on a closed bounded interval is integrable, and so is every bounded function with finitely many discontinuities. Integrability fails when different sample choices give different limits.

integrable — A function is integrable on an interval when the limit of its Riemann sums exists and is the same for every choice of sample points. Continuity on a closed bounded interval guarantees it.

\[ f \text{ continuous on } [a,b] \;\Longrightarrow\; f \text{ integrable on } [a,b] \]

The standard non-integrable example is the function that is 1 at rational inputs and 0 elsewhere. Choosing rational sample points gives every sum the value 1; choosing irrational ones gives 0, so no limit exists.

Figure (svg): What can be integrated, and one function that cannot

The right-hand example is the standard one: the sample points alone decide the answer, so no single limit exists.

OpenStax Calculus Volume 1, §5.2 The Definite Integral §5.2, pp. 469-476 — integrable functions

27. What is integrable, and what is not

Picture it

Two columns, with the standard counterexample.

Figure (svg): What can be integrated, and one function that cannot

The right-hand example is the standard one: the sample points alone decide the answer, so no single limit exists.

The failure is not that the function is strange to look at but that the sample points alone decide the answer. Without agreement between choices there is no single number to call the integral.

28. Worked example: a discontinuous but integrable function

Worked example

Example 5.13. A jump does not prevent integration.

\[ \text{Is the step function equal to } 1 \text{ on } [0,1) \text{ and } 2 \text{ on } [1,2] \text{ integrable?} \]

Note the discontinuity

Why: A jump at 1.

Check boundedness

Why: Values are 1 and 2.

Count the discontinuities

Why: One point.

Apply the criterion

Why: Bounded with finitely many jumps.

Compute the value

Why: Two rectangles.

\[ 1 + 2 = 3 \]

Figure (svg): What can be integrated, and one function that cannot

The right-hand example is the standard one: the sample points alone decide the answer, so no single limit exists.

\[ \int_{0}^{2}f = 1\cdot 1 + 2\cdot 1 = 3 \]

Verify: see why one point cannot matter

Why: Any subinterval containing the jump has width tending to zero, and the function is bounded there, so its contribution to the sum tends to zero however the sample point is chosen inside it. A single point has no width and therefore no area — which is why changing a function's value at finitely many points does not change its integral at all. The criterion of finitely many jumps is exactly this observation made general.

OpenStax Calculus Volume 1, §5.2 The Definite Integral §5.2, pp. 472-473

29. Integrable on [0,1]?

Sorting

Check boundedness and the discontinuities.

Sort into buckets

Sort each function.

Integrable
x^2; a step function with one jump; a bounded increasing function with many jumps but finitely many
Not integrable
1/x; 1 at rationals, 0 elsewhere
yes
Bounded, with at most finitely many discontinuities, so every sample choice gives the same limit.
no
Either unbounded on the interval, or discontinuous everywhere so that the sample choice decides the answer.

The reciprocal fails for a different reason from the last one: it is unbounded near zero rather than badly discontinuous. Both requirements — boundedness and few discontinuities — are genuinely needed.

30. Worked example: a function that is not integrable

Worked example

Checkpoint 5.13. The standard counterexample.

\[ \text{Show that the function equal to } 1 \text{ at rationals and } 0 \text{ elsewhere is not integrable on } [0,1]. \]

Choose rational sample points

Why: Every subinterval contains one.

\[ \text{all heights are } 1 \]

Compute that sum

Why: Total width times 1.

\[ 1,\text{ for every } n \]

Choose irrational sample points

Why: Every subinterval contains one too.

\[ \text{all heights are } 0 \]

Compute that sum

Why: Total width times 0.

\[ 0,\text{ for every } n \]

Conclude

Why: Two different limits.

Figure (svg): The solution to Worked example a function that is not integrable shown as a ladder of expressions, one row per legal move

The whole solution at once: each drop is one legal move.

\[ \lim = 1 \text{ or } 0, \text{ depending on the choice} \]

Verify: identify precisely which requirement failed

Why: The function is bounded, between 0 and 1, so boundedness was not the problem. What failed is the requirement that the limit be independent of the sample points — and this function is discontinuous at every point, not finitely many. The example is what forced mathematicians to state that independence requirement explicitly rather than assuming it, and it is why Section 5.1's theorem about agreement was worth proving.

OpenStax Calculus Volume 1, §5.2 The Definite Integral §5.2, pp. 473-474

31. Trap: assuming any discontinuity prevents integration

Trap

The trap

\[ f \text{ has a jump at } 1 \;\Longrightarrow\; \text{not integrable} \]

Reject the function

Why: The student overgeneralises from the counterexample.

A bounded function with finitely many jumps is integrable, because each jump sits in a subinterval whose width tends to zero.

The fix

\[ \text{bounded} + \text{finitely many discontinuities} \;\Longrightarrow\; \text{integrable} \]

Check boundedness and count the discontinuities

Why: Continuity is sufficient but not necessary.

The Dirichlet function fails because it is discontinuous EVERYWHERE, not because it is discontinuous somewhere. The distinction matters in applications, where measured data with occasional jumps is common and perfectly integrable.

32. Name the sufficient condition

Fill the middle

The simplest guarantee of integrability.

Fill in the blanks

f \textcontinuous \; ___ \text___ [a,b] \;\Longrightarrow\; f \text___

Why: Continuity on a closed bounded interval is sufficient. It is not necessary — step functions are integrable too — but it covers almost everything met in practice.

33. One of these claims is false

Two truths and a lie

All three are about integrability.

Eliminate the wrong options

Two of these are true. Knock those out and keep the false one.

  • A. Changing a function at finitely many points does not change its integral
  • C. The Dirichlet function is bounded yet not integrable
  • B. Every discontinuous function fails to be integrable

Survives elimination: B

Why: The survivor is the false one. Step functions are discontinuous and perfectly integrable, and so is any bounded function with finitely many jumps. What matters is whether the discontinuities are few enough that the sample choice cannot change the limit.

34. What exactly fails?

Prediction

Commit before reasoning.

Predict first

For the function that is 1 at rationals and 0 elsewhere, which requirement of the definition fails?

  • Boundedness
  • That the limit be the same for every choice of sample points
  • That the interval be closed
  • Nothing fails

Correct: That the limit be independent of the sample points.

\[ \text{rational choice} \to 1, \quad \text{irrational choice} \to 0 \]

Why: The function is bounded between 0 and 1, and the interval is perfectly ordinary. What fails is agreement: rational sample points give every sum the value 1 and irrational ones give 0, so there are two candidate limits and no single number to call the integral. This example is precisely why that independence clause appears in the definition at all.

35. The properties

Section

Section 4

36. Rules inherited from sums

Concept

Equal limits give zero, swapping the limits flips the sign, sums split, constants come outside, and adjacent intervals join. Each is the limit of the corresponding fact about finite sums.

the additive property — The integral over an interval equals the sum of the integrals over any two pieces meeting at a point, and the sign convention makes it hold even when that point lies outside the interval.

\[ \int_{a}^{b} = \int_{a}^{c} + \int_{c}^{b}, \qquad \int_{b}^{a} = -\int_{a}^{b} \]

The reversal rule is a definition rather than a theorem, chosen precisely so the additive property holds for every c. Without it the splitting rule would need a case distinction for every position of c.

Figure (svg): The properties of the definite integral, grouped by what they do

None of these needs a separate proof from scratch: each is the limit of a statement about finite sums.

OpenStax Calculus Volume 1, §5.2 The Definite Integral §5.2, pp. 474-482 — properties of the definite integral

37. Seven rules

Picture it

Each with its origin.

Figure (svg): The properties of the definite integral, grouped by what they do

None of these needs a separate proof from scratch: each is the limit of a statement about finite sums.

Only the second is a convention; the rest are theorems, and each is proved by writing the corresponding statement about Riemann sums and taking limits.

38. Worked example: using the properties

Worked example

Example 5.15. Combining several rules.

\[ \text{Given } \int_{0}^{3}f = 7 \text{ and } \int_{0}^{5}f = 12, \text{ find } \int_{5}^{3}f. \]

Split the larger interval

Why: At the interior point 3.

\[ \int 0\text{ to } 5 = \int 0\text{ to } 3 + \int 3\text{ to } 5 \]

Substitute the known values

Why: Two of the three are given.

\[ 12 = 7 + \int 3\text{ to } 5 \]

Solve

Why: Subtract.

\[ \int 3\text{ to } 5 = 5 \]

Apply the reversal rule

Why: Swapping the limits flips the sign.

\[ \int 5\text{ to } 3 = -5 \]

State

Why: The answer.

\[ -5 \]

Figure (svg): The properties of the definite integral, grouped by what they do

None of these needs a separate proof from scratch: each is the limit of a statement about finite sums.

\[ \int_{5}^{3}f = -5 \]

Verify: sanity-check the reversal and the split

Why: The reversal must flip the sign, so a positive integral from 3 to 5 gives a negative one from 5 to 3 — consistent. The split can be checked by adding back: 7 plus 5 gives 12, matching the given value over the whole interval. Note that neither the function nor its formula was ever needed, which is the point of having properties: they answer questions about integrals without computing any.

OpenStax Calculus Volume 1, §5.2 The Definite Integral §5.2, pp. 477-478

39. Reverse the limits

Fill the middle

A known integral, with the limits swapped.

Fill in the blanks

\int_-^___f = ___\int____^___f

Why: Swapping the limits flips the sign. This is a definition chosen so that the additive property holds for every splitting point, including ones outside the interval.

40. Worked example: comparison and bounding

Worked example

Example 5.17. An estimate without computing.

\[ \text{Bound } \int_{1}^{2}\frac{1}{x}\,dx \text{ without evaluating it.} \]

Find the function's range on the interval

Why: It decreases.

\[ \text{between } \frac{1}{2}\text{ and } 1 \]

Apply the lower bound

Why: Minimum times the width.

\[ \text{at least } \frac{1}{2} \]

Apply the upper bound

Why: Maximum times the width.

\[ \text{at most } 1 \]

State the bracket

Why: The width is 1.

\[ \frac{1}{2} \le\text{ integral } \le 1 \]

Compare with the true value

Why: It is the natural logarithm of 2.

\[ \text{about } 0.693 \]

Figure (svg): Comparison and bounding: one curve above another, and both between two lines

Bounding gives an integral's range without computing it, which is often all that a proof or an estimate needs.

\[ \tfrac12 \le \int_{1}^{2}\frac{dx}{x} \le 1 \]

Verify: check the bound is genuine and note its cost

Why: The true value of 0.693 sits comfortably inside. The bounding property cost two function evaluations and no integration at all, which is why it is used constantly in proofs and error estimates — often a bound is all that is needed, and it is available when the integral itself is not computable. Note the connection to Section 5.1's upper and lower sums: this is that idea with a single rectangle.

OpenStax Calculus Volume 1, §5.2 The Definite Integral §5.2, pp. 479-481

41. Find the error: the sign lost on reversal

Error analysis

A student uses a known integral with the limits the other way round.

Annotate

On: \( \int_{0}^{2}f = 5 \;\Longrightarrow\; \int_{2}^{0}f = 5 \)

  • The two integrals involve the same function over the same interval.
  • But swapping the limits flips the sign, by definition.
  • The correct value is -5.
  • The convention exists so that the additive property holds for every c, not only interior ones.

Watching the order of the limits is a habit worth building early, because Section 5.3's evaluation rule subtracts the value at the lower limit from the value at the upper one — and getting them the wrong way round negates every answer.

42. Property to its statement

Matching

The rules of the section.

Match the pairs

  • l1. equal limits
  • l2. swapped limits
  • l3. adjacent intervals
  • l4. one function above another
  • r1. the integral is zero
  • r2. the sign flips
  • r3. the integrals add
  • r4. its integral is at least as large

Why: The first is immediate — no width, no area — and the second is a convention. The last is the comparison property, and it is what makes bounding possible without any computation.

43. Which property settles this?

Sorting

Match the question to the rule.

Sort into buckets

Sort each question.

Equal limits
the integral from 3 to 3
Reversal
the integral from 5 to 2, given the one from 2 to 5
Additivity
the integral from 0 to 5, given those from 0 to 3 and 3 to 5
Bounding
a range for an integral with no formula available
Constant multiple
the integral of three times a function
zero
An interval of no width encloses no area.
flip
Swapping the order of the limits negates the value.
add
Integrals over adjacent intervals add to the integral over their union.
bound
The minimum and maximum of the function times the width bracket the value.
const
A constant factor passes outside the integral, exactly as it does outside a sum.

The fourth is the one worth remembering when a problem looks impossible: an integral with no elementary antiderivative can still be bracketed in two lines, and often a bracket is all that is wanted.

44. Why is reversal defined that way?

Prediction

Commit before reasoning.

Predict first

Why is the integral with swapped limits defined to be the negative rather than the same?

  • Arbitrarily
  • So that the additive property holds for every splitting point, including ones outside the interval
  • Because areas can be negative
  • To match derivatives

Correct: So that the additive property holds for every splitting point.

\[ \int_{a}^{b} = \int_{a}^{c}+\int_{c}^{b} \quad \text{for every } c, \text{ inside or outside} \]

Why: With the convention, the integral from a to b equals the sum of the integrals from a to c and c to b for ANY c — including one beyond b, where the second piece runs backwards and subtracts the excess. Without it the rule would need a case distinction for every position of c, and Section 5.3's evaluation formula would need one too. The convention is chosen to make later statements simple.

45. Average value

Section

Section 5

46. The height of an equal-area rectangle

Concept

The average value of a function over an interval is its integral divided by the interval's length — the constant height that would enclose the same area. A continuous function actually attains its average somewhere.

average value — The integral of a function over an interval, divided by the interval's length. It is the height of the rectangle with the same base and the same area.

\[ f_{\text{avg}} = \frac{1}{b-a}\int_{a}^{b}f(x)\,dx \]

That the value is attained is the Mean Value Theorem for Integrals, and it is the integral counterpart of Section 4.4's theorem — with the same hypothesis of continuity and the same kind of existence conclusion.

Figure (svg): The average value of a function as the height of an equal-area rectangle

That the function actually attains its average is a theorem — the Mean Value Theorem for Integrals — and it needs continuity.

OpenStax Calculus Volume 1, §5.2 The Definite Integral §5.2, pp. 482-488 — average value of a function

47. The equal-area rectangle

Picture it

A parabola and its average height.

Figure (svg): The average value of a function as the height of an equal-area rectangle

That the function actually attains its average is a theorem — the Mean Value Theorem for Integrals — and it needs continuity.

The rectangle at height four thirds encloses exactly the area under the curve, and the curve crosses that height once — which the theorem guarantees for any continuous function.

48. Worked example: computing an average value

Worked example

Example 5.18. Integral over width.

\[ \text{Find the average value of } f(x)=x^{2} \text{ on } [0,2]. \]

Recall the integral

Why: From Section 5.1.

\[ \frac{8}{3} \]

Compute the interval's length

Why: Two minus zero.

\[ 2 \]

Divide

Why: Integral over width.

\[ \frac{4}{3} \]

Interpret

Why: The equal-area rectangle's height.

\[ \text{about } 1.333 \]

Locate where it is attained

Why: Solve x squared equals four thirds.

\[ x\text{ about } 1.155 \]

Figure (svg): The average value of a function as the height of an equal-area rectangle

That the function actually attains its average is a theorem — the Mean Value Theorem for Integrals — and it needs continuity.

\[ f_{\text{avg}} = \frac{4}{3} \]

Verify: sanity-check the value against the function's range

Why: The function runs from 0 to 4 on this interval, so an average of 1.333 is plausible — and it is well below the midpoint of that range, which is right because the parabola spends most of the interval near its low values. Note the average is not the average of the endpoints, which would be 2; averaging a function means integrating it, not averaging a few of its values.

OpenStax Calculus Volume 1, §5.2 The Definite Integral §5.2, pp. 484-485

49. Divide by the width

Fill the middle

An integral of eight thirds over an interval of length two.

Fill in the blanks

f_4/3} = \frac______\cdot\frac______ = ___

Why: The average value is the integral divided by the interval's length. It is the height of the rectangle enclosing the same area over the same base.

50. Worked example: the Mean Value Theorem for Integrals

Worked example

Checkpoint 5.18. The average is attained.

\[ \text{State the theorem and say why continuity is needed.} \]

State the conclusion

Why: For a continuous function.

Note the average lies between the extremes

Why: By the bounding property.

\[ \min \le\text{ average } \le \max \]

Apply the Intermediate Value Theorem

Why: Section 2.4.

Conclude

Why: The average is such a value.

Test the necessity of continuity

Why: A step function jumping over its average.

Figure (svg): The solution to Worked example the Mean Value Theorem for Integrals shown as a ladder of expressions, one row per legal move

The whole solution at once: each drop is one legal move.

\[ \exists c\in[a,b]: \; f(c) = \frac{1}{b-a}\int_{a}^{b}f \]

Verify: build the counterexample that shows continuity is essential

Why: Take the function equal to 0 on the first half of an interval and 2 on the second. Its average is 1, and the function never takes the value 1 anywhere — it jumps straight past it. So the conclusion genuinely fails without continuity, and the proof shows exactly why: it used the Intermediate Value Theorem, which needs continuity. This is the same dependency pattern as Section 4.4's theorem.

OpenStax Calculus Volume 1, §5.2 The Definite Integral §5.2, pp. 485-487

51. Trap: the average taken over the endpoints

Trap

The trap

\[ f_{\text{avg}} = \frac{f(0)+f(2)}{2} = \frac{0+4}{2} = 2 \]

Average the two endpoint values

Why: The student treats it like averaging two numbers.

The true average is four thirds. Averaging endpoints ignores everything the function does in between.

The fix

\[ f_{\text{avg}} = \frac{1}{2}\int_{0}^{2}x^{2}dx = \frac{1}{2}\cdot\frac83 = \frac43 \]

Integrate and divide by the width

Why: The average of infinitely many values is an integral, not a finite mean.

The endpoint average is exactly what a single trapezoid would give, and the gap between 2 and four thirds measures how far the parabola sits below its chord. Averaging a function requires accounting for all of it.

52. Order the proof

Ranking

The Mean Value Theorem for Integrals.

Put in order

  1. Note the function is continuous on a closed interval
  2. Bound the integral by the minimum and maximum times the width
  3. Divide by the width to bracket the average between them
  4. Apply the Intermediate Value Theorem
  5. Conclude some point gives exactly the average

Why: Step d is where continuity is actually used, and it is why the theorem fails for step functions. The bounding in step b is the property from the previous idea, doing real work in a proof.

53. Does the function attain its average?

Sorting

Continuity is the deciding factor.

Sort into buckets

Sort each function on a closed interval.

Attains it
x^2 on [0,2]; sin x on [0, 2pi]; any continuous function
Need not
0 on the first half, 2 on the second; a step function jumping past its average
yes
Continuity plus the Intermediate Value Theorem forces every value between the extremes to be taken, including the average.
no
A jump can step straight over the average without ever equalling it.

The sine case is worth noticing: its average over a full period is zero, and it does attain zero — twice. A zero average does not mean the theorem has nothing to say.

54. Why is averaging an integral?

Prediction

Commit before reasoning.

Predict first

Why is the average of a function an integral rather than a mean of some values?

  • It is not
  • Because a function takes infinitely many values, and the integral is the limit of averaging n of them
  • Because integrals are easier
  • By convention

Correct: Because the integral is the limit of averaging n sample values.

\[ \frac{1}{n}\sum f(x_{i}) = \frac{1}{b-a}\sum f(x_{i})\Delta x \;\longrightarrow\; \frac{1}{b-a}\int_{a}^{b}f \]

Why: Averaging n equally spaced values means summing them and dividing by n, and multiplying and dividing by the width turns that into a Riemann sum divided by the interval's length. Taking n to infinity gives exactly the integral over the width. So the definition is not an analogy with finite averages but the actual limit of them, which is why it deserves the name.

55. Indefinite against definite

Comparison

Fill the blanks. The two objects are different in kind.

Comparison matrix

Indefinite integralDefinite integral
Resulta family of functionsa single number
Carries a constantyes, the plus Cno
The variablesurvives in the answervanishes: it is a placeholder
Answerswhat has this derivative?what is the net signed area?

The two look alike and answer unrelated questions. Section 5.3's theorem is startling precisely because it connects them, and until then nothing suggests they should be related at all.

56. The procedure, in order

Pattern

Given a question about a definite integral.

  1. Check whether the question wants net signed area or total area, since the integral gives the first.
  2. For total area, find the integrand's zeros, split there, and add the magnitudes of the pieces.
  3. Use the properties before computing: equal limits give zero, reversal flips the sign, and adjacent intervals join.
  4. When only a range is needed, bound the integral by the function's minimum and maximum times the width.
  5. For an average value, integrate and divide by the interval's length, not by the number of points sampled.

Step one is the one that decides whether an answer is right or answers a different question. An area question whose answer comes out negative or zero has almost certainly skipped it.

Stewart, Calculus: Early Transcendentals 8e, §5.2 The Definite Integral §5.2, pp. 378-391

57. Check yourself 1 of 3

Check

Signed area.

Check your understanding

The integral of sin x from 0 to 2pi is zero. What is the total area between the curve and the axis?

  • A. 4 (correct)
  • B. 0
  • C. 2
  • D. It cannot be determined

Answer: A

Why: Each half has area 2, and total area counts both positively.

Why B tempts people
This is the signed value, in which the two halves cancelled.
Why C tempts people
This is one half of the region only.
Why D tempts people
It is entirely determined: split at pi and add magnitudes.

58. Check yourself 2 of 3

Check

Properties.

Check your understanding

If the integral of f from 2 to 5 is 5, what is the integral from 5 to 2?

  • A. -5 (correct)
  • B. 5
  • C. 0
  • D. 1/5

Answer: A

Why: Swapping the limits flips the sign, by definition.

Why B tempts people
This ignores the reversal convention, which exists to make the additive property universal.
Why C tempts people
Zero would require equal limits, not swapped ones.
Why D tempts people
Reversal negates; it does not take a reciprocal.

59. Check yourself 3 of 3

Check

Average value.

Check your understanding

The integral of x^2 from 0 to 2 is 8/3. What is the function's average value there?

  • A. 4/3 (correct)
  • B. 8/3
  • C. 2
  • D. 16/3

Answer: A

Why: Divide the integral by the interval's length of 2.

Why B tempts people
This is the integral itself, not the average.
Why C tempts people
This averages the two endpoint values, ignoring everything between them.
Why D tempts people
This multiplies by the width rather than dividing.

60. Where this shows up outside the textbook

Real world

A tidal turbine's power output is positive when the tide flows in and negative when it draws power to reposition during slack water. Over a twelve-hour cycle the operator has a continuous power curve.

Discussion prompt

Explain what the integral of power over the cycle gives, how it differs from the total energy handled, and what the average value means.

Hint: Power integrated over time is energy, and the sign records direction.

Answer:

The integral of power over the cycle gives the net energy delivered — generation minus consumption — because the negative stretches genuinely subtract. That is the number the operator gets paid on, and the signed convention is exactly right for it.

\[ E_{\text{net}} = \int_{0}^{12}P(t)\,dt \]

The total energy handled is a different quantity, found by splitting at the zeros of the power curve and adding magnitudes. It matters for a different reason: it determines wear on the mechanism, which does not care about direction. A turbine with zero net output can still be working hard.

The average value is the net energy divided by twelve hours — the constant power output that would deliver the same net energy over the cycle. It is the honest figure to quote for a capacity comparison, and it is generally far below the peak, which is why turbine ratings quoted as peak power are misleading.

Note that all three numbers come from the same curve and answer different questions, and that confusing them has real consequences: quoting the peak sells the turbine, quoting the average describes it, and quoting the net signed value is what the electricity meter reads.

61. How sure are you?

Commit first

Answer, then rate your confidence honestly.

Predict first

An area question produces an integral equal to zero. What is the most likely explanation?

  • The region is empty
  • The integrand changes sign, and the positive and negative parts cancelled
  • The integral was computed wrongly
  • The function is not integrable

Correct: The integrand changes sign and the parts cancelled.

\[ \int_{0}^{2\pi}\sin x\,dx = 0, \quad \text{total area} = 4 \]

Why: The integral gives net signed area, so any region with as much below the axis as above returns zero. That is the correct value of the integral and the wrong answer to an area question — total area needs the integrand split at its zeros and the magnitudes added. An answer of zero to an area question is a reliable warning sign, since a genuinely empty region is rarely what a problem is about.

62. Explain it to someone a year behind you

Explain it

They computed the integral of the sine over a full period, got zero, and concluded the area under a sine wave is nothing.

Discussion prompt

In four sentences or fewer, sort them out.

Hint: Ask them to sketch it.

Answer:

Have them sketch the curve: there is clearly a hump above the axis and an equal one below. The integral counts the lower hump negatively, so the two cancel — that is what a signed area does, and the answer of zero is correct for what the integral measures.

For the region's actual size, split at pi, integrate each half, and add the magnitudes to get 4. The rule of thumb is that an area question answered with zero or a negative number has skipped the split.

63. Exit ticket

Exit ticket

Name the weakest spot before you close the deck.

Predict first

Which of these would you least want handed to you cold?

  • Reading a Riemann sum back into an integral
  • Signed area against total area
  • The properties, especially reversal and additivity
  • Average value and the theorem behind it

Correct: Whichever you picked is tonight's ten minutes, and each has a one-line fix.

Why: For reading sums, the width factor tells you the interval length. For area, always ask which question is being posed before computing. For properties, remember reversal is a convention chosen to make additivity universal. For averages, divide by the width and remember the theorem needs continuity. Do five of your chosen kind rather than twenty mixed ones.

64. Draw the lesson on one page

Connect it up

Paper. Fifteen minutes.

Draw it

At the top, write the definition as a limit of Riemann sums with an arrow to the integral notation, and label every symbol with where it came from. Below, sketch a full sine period with the upper region shaded one way and the lower another, and write both the integral and the total area beside it with one line saying why they differ. In the middle, list the seven properties, marking which one is a convention rather than a theorem and writing in a few words why that convention was chosen. Beside them, work one problem using additivity and reversal together. In the lower half, sketch a parabola with its average-value rectangle drawn to the same area, mark where the curve crosses that height, and write the Mean Value Theorem for Integrals with its hypothesis. At the bottom, write the counterexample showing why continuity is needed there, and one line on what makes a function fail to be integrable.

If your average-value rectangle looks taller than the area under the curve, redraw it — the two regions must be equal by construction, and getting that visibly right is what makes the definition memorable.

65. What you can do now

Recap

Five things, and none of them yet needs an antiderivative.

If you seeThen
A limit of Riemann sumsRead off the interval from the width factor
An area questionSplit at the zeros before integrating
A zero answer to an area questionThe signs cancelled; split and retry
Limits the wrong way roundFlip them and negate
Adjacent intervalsTheir integrals add
An integral you cannot computeBound it by the extremes times the width
The word averageIntegrate and divide by the width

Section 5.3 is the chapter's centre. It proves that this limit of sums is computed by an antiderivative evaluated at the two endpoints — connecting Chapter 4 to Chapter 5 and making almost every integral in this deck a two-line calculation.

OpenStax Calculus Volume 1, §5.2 The Definite Integral §5.2, pp. 456-471 — everything on these slides traces back here

Sources

  1. OpenStax Calculus Volume 1, §5.2 The Definite Integral — Strang & Herman, OpenStax / Rice University, CC BY-NC-SA 4.0, pp. 456-471
  2. Stewart, Calculus: Early Transcendentals 8e, §5.2 The Definite Integral — James Stewart, Cengage Learning, 2016, pp. 378-391

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