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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).

Move xx and watch F(x)=∫axf(t) dtF(x)=\int_a^x f(t)\,\mathrm{d}t being drawn below; its slope at xx is f(x)f(x). Where ff jumps, FF is still continuous but gets a corner.

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