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Fundamental Theorem of Calculus Part 2

Theorem

Suppose a<ba < b are real numbers, and let f ⁣:[a,b]→Rf\colon [a, b] \to\mathbb{R} be a Riemann integrable function. If F ⁣:[a,b]→RF\colon [a, b] \to\mathbb{R} is an antiderivative of f,f\text{,} then

∫abf(x) dx=F(x)∣x=ab=F(b)−F(a).\int_a^b f(x)\,\mathrm{d}x =F(x)\big|_{x=a}^{b}=F(b)-F(a).

Interpretation

This part of the fundamental theorem turns the evaluation of a definite integral into a subtraction. Once an antiderivative FF of ff is known, the limit of Riemann sums equals F(b)−F(a)F(b)-F(a), and no sums have to be computed.

Two panels: the area under f from a to b, and the graph of an antiderivative F whose rise from F(a) to F(b) equals that area.

The figure uses f(x)=x/2f(x)=x/2 and F(x)=x2/4F(x)=x^2/4, with a=1a=1 and b=3b=3. The area in the left panel is 22, while the right panel rises by F(3)−F(1)=9/4−1/4=2F(3)-F(1)=9/4-1/4=2. The theorem equates these two quantities. Where ff is large, FF climbs steeply, and where ff is small, FF is nearly flat. This example has f≥0f\ge0; for an integrand that changes sign, the integral measures signed area.

The reason is a telescoping sum. For a partition PP, the mean value theorem gives points cic_i with F(xi)−F(xi−1)=f(ci)(xi−xi−1)F(x_i)-F(x_{i-1})=f(c_i)(x_i-x_{i-1}). With these tags the Riemann sum is exactly F(b)−F(a)F(b)-F(a), for every PP, so the integral is F(b)−F(a)F(b)-F(a) as well.

Both hypotheses are needed. The integral must exist: F(x)=x2sin⁡(1/x2)F(x)=x^2\sin(1/x^2) with F(0)=0F(0)=0 is differentiable on [0,1][0,1], but F′F' is unbounded near 00 and therefore not Riemann integrable. And FF must be an antiderivative on all of [a,b][a,b]. The function −arctan⁡(1/x)-\arctan(1/x) has derivative 11+x2\frac{1}{1+x^2} for x≠0x\ne0, yet its difference between x=1x=1 and x=−1x=-1 is −π2-\frac{\pi}{2}, while ∫−11dx1+x2=π2\int_{-1}^{1}\frac{\mathrm{d}x}{1+x^2}=\frac{\pi}{2}; it jumps at 00, so the theorem does not apply to it.

Later, the rules of integration by parts and substitution combine this theorem with the product rule and the chain rule.


Key Results

  • Definite integrals can be evaluated using antiderivatives.
  • The result depends only on boundary values.
  • Integration becomes an algebraic operation once antiderivatives are known.

Examples

  • ∫01x2 dx=13.\displaystyle \int_0^1 x^2\,\mathrm{d}x=\frac{1}{3}\text{.}
  • ∫ab1 dx=b−a.\displaystyle \int_a^b 1\,\mathrm{d}x=b-a\text{.}

Prerequisites

Sources

Aliases: FTC 2, second fundamental theorem of calculus, Newton-Leibniz formula, Newton-Leibniz theorem Symbols: integral, pi, real numbers

Last updated: 27 October 2026 11:52