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Worked Example

01006030 | Week 9 | Lecture Notes

Fundamental Theorem & Substitution

The theorem that gives calculus its name: derivatives and integrals, Weeks 2-4 and Week 7's seemingly separate limits, turn out to be inverse operations. Then the first systematic technique for computing integrals that are not immediately obvious.

Welcome back from the midterm. Week 7 left the derivative and the definite integral looking like two unrelated limits — one about tangent slopes, one about area. This week proves they are inverse processes, which is the single most useful fact in the whole course: it replaces the Riemann-sum limit of Week 7 with ordinary antidifferentiation for nearly every integral you will ever compute by hand.

9.1 The Fundamental Theorem, Part 1

Define F(x) = ∫ax f(t) dt — the integral from a fixed point a to a variable upper limit x. If f is continuous, then

F′(x) = f(x) (9.1)

In words: differentiating an integral with respect to its upper limit gives back the original integrand. The rate at which accumulated area grows, at x, is exactly the height of the curve there — the derivative undoes the integral.

Example 9.1 — Applying FTC Part 1 directly

Find d/dx ∫2x √(1+t3) dt.

Step 1 — Recognise the form of Eq. 9.1

Here f(t) = √(1+t3), a continuous function, and the upper limit is x itself.

Step 2 — Apply the theorem

d/dx ∫2x √(1+t3) dt = √(1+x3) — no antiderivative was ever computed.

When the upper limit is itself a function g(x) rather than plain x, the Chain Rule (Week 4 §4.10) attaches automatically:

d/dx ∫ag(x) f(t) dt = f(g(x))·g′(x) (9.2)

9.2 The Fundamental Theorem, Part 2

If f is continuous on [a,b] and F is any antiderivative of f (meaning F′=f), then

∫ab f(x) dx = F(b) − F(a) (9.3)

written F(x)]ab. This is the practical half: it replaces the Riemann-sum limit of Week 7 §7.5 with "find any antiderivative, then subtract" — no limits, no sums.

Example 9.2 — Recomputing Week 7's integral instantly

Evaluate ∫02 x2 dx using FTC Part 2, and compare to the limit computation in Week 7, Example 7.2.

Step 1 — Find any antiderivative of x²

F(x) = x3/3 works, since F′(x) = x2.

Step 2 — Apply Eq. 9.3

F(2) − F(0) = 8/3 − 0

= 8/3, matching the limit-of-Riemann-sums answer from Week 7 exactly — without a single sum or limit computed this time.

9.3 Why the Two Parts Fit Together

Part 1 says the derivative of an integral (with a variable upper limit) recovers the integrand. Part 2 says the integral can be evaluated using any antiderivative. Together they say differentiation and integration are inverse operations — the same relationship as f and f−1 undoing each other, but for the two central operations of calculus rather than for numbers.

9.4 Indefinite Integrals and Antiderivative Families

The indefinite integral ∫ f(x) dx denotes the entire family of antiderivatives of f, not a single function or a number:

∫ f(x) dx = F(x) + C (9.4)

where F′=f and C is an arbitrary constant. This is exactly the consequence of the Mean Value Theorem from Week 6 §6.5: any two antiderivatives of the same function differ only by a constant, so once one is found, all of them are known.

9.5 Basic Antiderivative Formulas

Each differentiation formula from Weeks 4 and 4.9 reads backwards as an antiderivative formula:

∫ xn dx = xn+1n+1 + C,   n ≠ −1 (9.5a)
∫ sin x dx = −cos x + C (9.5b)
∫ cos x dx = sin x + C (9.5c)
∫ sec2x dx = tan x + C (9.5d)

The restriction n ≠ −1 in Eq. 9.5a leaves a gap — ∫ x−1 dx — that Week 11 fills once the natural logarithm is introduced.

9.6 The Substitution Method for Indefinite Integrals

Substitution is the antiderivative counterpart of the Chain Rule, and is often called u-substitution. To integrate a composite structure, name the inner function u = g(x), compute du = g′(x)dx, and rewrite the whole integral in terms of u alone.

Example 9.3 — Substitution, indefinite integral

Evaluate ∫ 2x cos(x2) dx.

Step 1 — Choose u to be the inner function

u = x2, so du = 2x dx — which is exactly the factor sitting next to cos(x2).

Step 2 — Rewrite entirely in terms of u

∫ 2x cos(x2) dx = ∫ cos u du

Step 3 — Integrate in u, then substitute back

sin u + C

= sin(x2) + C

The test for whether substitution will work

Substitution succeeds exactly when, after choosing u, every remaining piece of the integral — not just some of it — can be rewritten purely in terms of u (including dx itself, via du). If a leftover x cannot be eliminated, the chosen u was wrong, or the integral needs a different technique (Week 12).

9.7 Substitution in Definite Integrals

For a definite integral, substitution has an extra bookkeeping step: the limits of integration must also convert from x-values to the corresponding u-values, so that the final evaluation never needs to substitute back to x at all.

Example 9.4 — Substitution, definite integral

Evaluate ∫01 x√(x2+1) dx.

Step 1 — Substitute and convert the limits

u = x2+1, du = 2x dx, so x dx = du/2. At x=0, u=1; at x=1, u=2.

Step 2 — Rewrite the whole integral in u, including the limits

∫12 √u (du/2) = (1/2)∫12 u1/2 du

Step 3 — Integrate and evaluate directly in u (no back-substitution needed)

(1/2)·(2/3)u3/2]12 = (1/3)(23/2−1)

= (2√2 − 1)/3

9.8 The Area Between Two Curves

If f(x) ≥ g(x) on [a,b], the area between the curves is

A = ∫ab [f(x) − g(x)] dx (9.6)

— always the top curve minus the bottom curve, so the integrand stays non-negative and the answer is a genuine (unsigned) area, even when part of the region dips below the x-axis.

Example 9.5 — Area between two curves

Find the area of the region bounded by y=x2 and y=x+2.

Step 1 — Find the intersection points (the limits of integration)

x2 = x+2  ⇒  x2−x−2=0  ⇒  (x−2)(x+1)=0  ⇒  x=−1, 2.

Step 2 — Determine which curve is on top

At x=0 (inside the interval): line gives 2, parabola gives 0, so the line is on top.

Step 3 — Apply Eq. 9.6 and evaluate

A = ∫−12 [(x+2) − x2] dx = [x2/2 + 2x − x3/3]−12

At x=2: 2+4−8/3 = 10/3. At x=−1: 1/2−2+1/3 = −7/6.

A = 10/3 − (−7/6) = 20/6+7/6 = 27/6 = 9/2

9.9 Worked Capstone Example

Example 9.6 — Combining FTC Part 1, the Chain Rule, and substitution

Find h′(x) for h(x) = ∫1x2 sin(√t) dt, then verify the underlying integral could also be attacked with substitution.

Step 1 — Apply Eq. 9.2 (FTC Part 1 with a function upper limit)

h′(x) = sin(√x2)·d/dx[x2] = sin(x)·2x, using √x2=x for x ≥ 0.

h′(x) = 2x sin x

Step 2 — Note the substitution structure inside the integral itself

Inside ∫ sin(√t) dt, the substitution u=√t (so t=u2, dt=2u du) converts it into ∫ 2u sin u du — not elementary by the formulas in §9.5 alone (it needs integration by parts, Week 12), which is exactly why FTC Part 1 was the efficient route here: it never required finding this antiderivative at all.

9.10 Nomenclature

SymbolMeaning
FTCFundamental Theorem of Calculus
∫ f(x)dxIndefinite integral: the family of antiderivatives of f
CConstant of integration
u-substitutionRewriting an integral in a new variable u=g(x) to reverse the Chain Rule
F(x)]abShorthand for F(b) − F(a)

9.11 Problems

  1. FTC Part 1. Find d/dx ∫0x t3 dt.
  2. FTC Part 1 with the Chain Rule. Find d/dx ∫0sin x √(1+t2) dt.
  3. FTC Part 2. Evaluate ∫14 (3x2−2x) dx.
  4. Indefinite integral. Find ∫ (4x3 − sec2x) dx.
  5. Substitution, indefinite. Evaluate ∫ x2(x3+1)4 dx.
  6. Substitution, trig. Evaluate ∫ sin3x cos x dx.
  7. Substitution, definite. Evaluate ∫01 3x2√(x3+1) dx.
  8. Area between curves, i. Find the area bounded by y=x2 and y=4.
  9. Area between curves, ii. Find the area bounded by y=x3 and y=x for x∈[0,1].
  10. Combined. Find the area bounded by y=√x and y=x2, using substitution if needed during the integration step.

9.12 References