Skip to content

Fundamental Theorem of Calculus Part 1

Theorem

Suppose a<ba < b are real numbers, f ⁣:[a,b]→Rf\colon [a, b] \to\mathbb{R} is a Riemann integrable function, and F ⁣:[a,b]→RF\colon [a, b] \to\mathbb{R} is the function defined as:

F(x)=∫axf(t) dt.F(x)=\int_a^x f(t)\,\mathrm{d}t.

Then, FF is continuous on [a,b].[a,b]\text{.} Moreover, if x0∈(a,b)x_0\in(a,b) and ff is continuous at x=x0,x=x_0\text{,} then FF is differentiable at x=x0,x=x_0\text{,} with F′(x0)=f(x0).F'(x_0)=f(x_0)\text{.}


Interpretation

Integrating ff from aa up to a moving point xx produces a new function FF, and this part of the fundamental theorem describes how FF changes: it is always continuous, and where ff is continuous its rate of change is the current value f(x)f(x). In this sense differentiation undoes integration.

The area under a curve from a to x shaded as F(x), and a thin extra strip from x to x + h of area about f(x) times h, showing that F'(x) = f(x).

The figure shows why. Moving the right edge from xx to x+hx+h adds the thin red strip, whose area F(x+h)−F(x)F(x+h)-F(x) is about f(x) hf(x)\,h for small hh. Dividing by hh and letting h→0h\to0 gives F′(x)=f(x)F'(x)=f(x). The approximation becomes exact in the limit because ff is continuous at xx, so its values on the strip are all close to f(x)f(x).

The two conclusions need different hypotheses. Continuity of FF needs only integrability: a Riemann integrable ff is bounded, say ∣f∣≤M|f|\le M, and then ∣F(x)−F(y)∣≤M∣x−y∣|F(x)-F(y)|\le M|x-y|. The derivative statement needs continuity of ff at x0x_0. Where ff jumps, FF has a corner and is not differentiable. Even a change at a single point matters: if f(1)=1f(1)=1 and f(x)=0f(x)=0 otherwise on [0,2][0,2], then FF is identically 00, so F′(1)=0≠f(1)F'(1)=0\ne f(1).

The theorem shows that every continuous function on an interval has an antiderivative, namely FF, and part 2 then turns integrals into differences F(b)−F(a)F(b)-F(a).


Key Results

  • Integration defines a continuous function.
  • Differentiation recovers the original integrand at points of continuity.
  • The theorem establishes a local connection between integration and differentiation.

Examples

  • If f(x)=x2,f(x)=x^2\text{,} then F(x)=∫0xt2 dt\displaystyle F(x)=\int_0^x t^2\,\mathrm{d}t and F′(x)=x2.F'(x)=x^2\text{.}
  • For variable limits, suppose gg and hh are differentiable at xx, their values stay in [a,b][a,b] near xx, and ff is continuous at both g(x)g(x) and h(x)h(x). Then:

    ddx∫g(x)h(x)f(t) dt=h′(x)f(h(x))−g′(x)f(g(x)).\frac{\mathrm{d}}{\mathrm{d}x}\int_{g(x)}^{h(x)}f(t)\,\mathrm{d}t=h'(x)f(h(x)) -g'(x)f(g(x)).

Prerequisites

Sources

Aliases: FTC 1, first fundamental theorem of calculus Symbols: element of, integral, real numbers

Last updated: 22 October 2026 19:04