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Integral calculus theorems

Fundamental Theorem of Calculus Part 2: Evaluating Integrals

FTC part 2: the definite integral of f from a to b equals F(b) − F(a) for any antiderivative F. Statement, graph, a key counterexample and worked examples.

Integral calculus theorems Updated 3 min read

At a glance

\int_a^b f(x)\,dx = F(b) - F(a)
Also called
Evaluation theorem, Newton-Leibniz formula
Hypotheses
f is continuous on [a, b], and F is any antiderivative of f there (F' = f)
Conclusion
\int_a^b f(x)\,dx = F(b) - F(a)
Notation
\big[F(x)\big]_a^b = F(b) - F(a)
Net change form
\int_a^b F'(x)\,dx = F(b) - F(a)
Course
Calculus 1
On this page
  1. Statement of FTC part 2
  2. What FTC 2 means
  3. Why continuity matters
  4. Worked examples
  5. Common mistakes
  6. How FTC 2 connects to FTC 1

The fundamental theorem of calculus, part 2 (FTC 2), also called the evaluation theorem, says that a definite integral can be computed by finding an antiderivative and subtracting its values at the endpoints. It replaces the limit of Riemann sums with one line of algebra.

Statement of FTC part 2

Suppose that

  1. f is continuous on [a, b], and
  2. F is any antiderivative of f on [a, b], so F'(x) = f(x).

Then

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

The right side is often written \big[F(x)\big]_a^b or F(x)\Big|_a^b.

What FTC 2 means

The definite integral adds up f(x)\,dx across the interval. If f is the rate of change of F, adding up all the small changes F'(x)\,dx gives the total change in F, which is F(b) - F(a). This is the net change theorem: integrate velocity to get displacement, integrate a flow rate to get the total volume.

FTC part 2: area under y = sin(x) from 0 to π equals 2
With antiderivative F(x) = -\cos x, the shaded area is F(\pi) - F(0) = 1 - (-1) = 2.

Why continuity matters

Consider \int_{-1}^{1}\frac{1}{x^2}\,dx. An antiderivative of x^{-2} is -\frac{1}{x}, and blindly applying the formula gives

\left[-\frac{1}{x}\right]_{-1}^{1} = -1 - 1 = -2

But \frac{1}{x^2} > 0 everywhere, so its integral cannot be negative. The mistake: \frac{1}{x^2} is not continuous on [-1, 1] because it blows up at x = 0, so FTC 2 does not apply. Treated correctly as an improper integral, it diverges to \infty. Always check for discontinuities inside the interval before plugging in.

Worked examples

Example 1: a polynomial. Evaluate \int_1^3 (2x + 1)\,dx.

Step 1. An antiderivative is F(x) = x^2 + x.

Step 2. F(3) = 9 + 3 = 12 and F(1) = 1 + 1 = 2.

Step 3. \int_1^3 (2x + 1)\,dx = 12 - 2 = 10.

Check with geometry: the region is a trapezoid with parallel sides f(1) = 3 and f(3) = 7 and width 2, so its area is \frac{3 + 7}{2}\cdot 2 = 10.

Example 2: a trig integral. Evaluate \int_0^\pi \sin x\,dx.

\int_0^\pi \sin x\,dx = \big[-\cos x\big]_0^\pi = -\cos\pi - (-\cos 0) = 1 + 1 = 2

This is the area under one arch of the sine curve, shown in the graph above.

Example 3: a logarithm. Evaluate \int_1^e \frac{1}{x}\,dx.

\frac{1}{x} is continuous on [1, e], and an antiderivative is \ln x. So

\int_1^e \frac{1}{x}\,dx = \ln e - \ln 1 = 1 - 0 = 1

Example 4: net change. A tank fills at r(t) = 3t^2 liters per minute. Between t = 1 and t = 2 minutes the volume increases by

\int_1^2 3t^2\,dt = \big[t^3\big]_1^2 = 8 - 1 = 7 \text{ liters}

Common mistakes

  1. Subtracting in the wrong order. It is F(b) - F(a), upper limit first.
  2. Dropping parentheses. With F(x) = x^2 - 3x, write F(b) - F(a) = (b^2 - 3b) - (a^2 - 3a). Losing the parentheses flips signs.
  3. Ignoring discontinuities. As shown above, an integrand that blows up inside [a, b] needs improper integral techniques.
  4. Confusing area with signed area. FTC 2 gives the signed area: regions below the x-axis count as negative. For total area, split where f changes sign, as in area between curves.

How FTC 2 connects to FTC 1

FTC part 1 says G(x) = \int_a^x f(t)\,dt is an antiderivative of f. Any other antiderivative differs from G by a constant (a consequence of the mean value theorem), so F(b) - F(a) = G(b) - G(a) = \int_a^b f(t)\,dt. That is the whole proof of part 2.

To find antiderivatives, see antiderivatives and u-substitution. For both parts of the theorem with more examples, read the fundamental theorem of calculus guide.

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Frequently asked questions

What does the second fundamental theorem of calculus say?

If f is continuous on [a, b] and F is any antiderivative of f, then \int_a^b f(x)\,dx = F(b) - F(a). A definite integral can be computed from an antiderivative instead of a limit of Riemann sums.

Why don't you need the +C in a definite integral?

If you use F(x) + C, the result is (F(b) + C) - (F(a) + C) = F(b) - F(a). The constant cancels, so any antiderivative gives the same answer.

Can the fundamental theorem of calculus give a wrong answer?

Only if you ignore its hypothesis. For \int_{-1}^{1}\frac{1}{x^2}\,dx the naive calculation gives -2, which is impossible for a positive integrand. The integrand is not continuous at 0, so the theorem does not apply and the integral actually diverges.

Is the fundamental theorem of calculus part 1 or part 2 used to evaluate integrals?

Part 2. Part 1 is about differentiating an integral with a variable limit, while part 2 is the F(b) - F(a) formula used to evaluate definite integrals.

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