Calculus I · The Fundamental Theorem of Calculus

The payoff: areas become subtractions

Part 1 says the area function is an antiderivative of ff. But antiderivatives are easy to find — just reverse the Chapter 4 rules — and they all differ by a constant (Chapter 6’s Mean Value Theorem, via Chapter 10’s +C+C). Chain those two facts together and the laborious definite integral collapses into arithmetic.

Figure 11.5
Figure 11.5

Fundamental Theorem of Calculus, Part 2. If ff is continuous and FF is any antiderivative of ff (any function with F′=fF' = f), then ∫abf(x)dx=F(b)−F(a).\int_a^b f(x)\,dx = F(b) - F(a).

Why it’s true. The area function A(x)=∫axfA(x) = \int_a^x f is one antiderivative (Part 1). Your FF is another, so they differ by a constant: F(x)=A(x)+CF(x) = A(x) + C. Then F(b)−F(a)=(A(b)+C)−(A(a)+C)=A(b)−A(a)=A(b)−0=∫abf(x)dx,F(b) - F(a) = \big(A(b)+C\big) - \big(A(a)+C\big) = A(b) - A(a) = A(b) - 0 = \int_a^b f(x)\,dx, since A(a)=∫aaf=0A(a) = \int_a^a f = 0. The constant cancels; any antiderivative works. ◼\blacksquare

We write F(b)−F(a)F(b) - F(a) as [F(x)]ab\big[F(x)\big]_a^b. And now watch Chapter 10’s hardest computation evaporate. There, finding ∫01x2dx\int_0^1 x^2\,dx took a page of Riemann sums and the sum-of-squares formula. Here:

∫01x2dx=[x33]01=133−033=13.\int_0^1 x^2\,dx = \left[\frac{x^3}{3}\right]_0^1 = \frac{1^3}{3} - \frac{0^3}{3} = \frac13.

Five seconds. Find an antiderivative, plug in the endpoints, subtract. Every area you can find an antiderivative for is now this easy: ∫0πsin⁡xdx=[−cos⁡x]0π=−cos⁡π+cos⁡0=1+1=2\int_0^\pi \sin x\,dx = [-\cos x]_0^\pi = -\cos\pi + \cos 0 = 1 + 1 = 2; ∫121xdx=[ln⁡|x|]12=ln⁡2\int_1^2 \tfrac1x\,dx = [\ln|x|]_1^2 = \ln 2.

The miracle, stated plainly

Stand back and see what just happened. Differentiation and integration are inverse operations — the two engines we built in total isolation, one measuring slopes and one measuring areas, are a single engine running in opposite directions. Part 1 says: integrate, then differentiate, and you return to where you started (ddx∫axf=f\tfrac{d}{dx}\int_a^x f = f). Part 2 says: to integrate, just undo a derivative. Slope and area, which have no visible relationship, turn out to be reciprocal questions. That two such different ideas are secretly the same is the reason calculus is not two subjects but one, and it is the engine under essentially all of physics, engineering, and quantitative science.

Figure 11.3
Figure 11.3

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