What is Calculus II

the Fundamental Theorem
of Calculus?

The bridge connecting differentiation and integration — proving they are inverse operations and making definite integrals computable in seconds.

Before this theorem, differentiation and integration looked like two completely separate inventions. Derivatives measure rates of change; integrals measure accumulated area. Why would those be related?

The Fundamental Theorem of Calculus (FTC) reveals they are exact inverses of each other — just as addition and subtraction are inverses, or multiplication and division. This single insight transformed calculus from a collection of clever techniques into a unified, powerful theory.

It has two parts. Part 1 says that differentiation undoes integration. Part 2 gives you a practical formula: to compute a definite integral, find any antiderivative and evaluate it at the two endpoints.

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Speed and distance — the perfect analogy

If \(v(t)\) is your speed at time \(t\), the integral \(\int_a^b v(t)\,dt\) gives your total distance travelled from time \(a\) to \(b\). But distance is also position \(s(t)\) — and \(v(t) = s'(t)\). So the integral of the derivative gives back the original quantity's net change: \(s(b) - s(a)\). That's the FTC in your car every day.

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Two operations that cancel

Differentiate then integrate: you get back (almost) what you started with. Integrate then differentiate: you get back exactly what you started with. The FTC makes this precise — and it's why antiderivatives are the key to computing areas. Without the FTC, you'd have to compute Riemann sums by hand for every integral.

Part 1
Differentiation of an Integral
$$\frac{d}{dx}\int_a^x f(t)\,dt = f(x)$$
If you define a function by integrating \(f\) from a fixed point \(a\) to a variable upper limit \(x\), then differentiating that function gives you back \(f(x)\). Integration and differentiation cancel out.
Part 2
Evaluating Definite Integrals
$$\int_a^b f(x)\,dx = F(b) - F(a)$$
If \(F\) is any antiderivative of \(f\) (i.e. \(F' = f\)), then the definite integral from \(a\) to \(b\) equals \(F(b) - F(a)\). No Riemann sums needed — just plug in the endpoints.
3.0
Shaded area = ∫₀ᵇ sin(x) dx = F(b) − F(0). Drag slider to change b.

To evaluate \(\displaystyle\int_1^3 x^2\,dx\):

1
Find an antiderivative \(F(x)\)
Use the power rule in reverse: \(F(x) = \dfrac{x^3}{3}\). (No need to add \(+C\) — it cancels.)
2
Write bracket notation
\(\Big[\dfrac{x^3}{3}\Big]_1^3\)
3
Evaluate at upper bound
\(F(3) = \dfrac{27}{3} = 9\)
4
Subtract lower bound value
\(F(1) = \dfrac{1}{3}\)  →  Answer: \(9 - \dfrac{1}{3} = \dfrac{26}{3}\)
Example 1 — Basic
\(\displaystyle\int_0^2 3x^2\,dx\)
\(F(x)=x^3\)
\([x^3]_0^2 = 8 - 0 = 8\)
Example 2 — Trig
\(\displaystyle\int_0^{\pi} \sin x\,dx\)
\(F(x)=-\cos x\)
\(-\cos\pi+\cos 0 = 1+1 = 2\)
Example 3 — Part 1
\(\dfrac{d}{dx}\displaystyle\int_0^x e^{t^2}\,dt\)
By FTC Part 1:
\(= e^{x^2}\) directly
Example 4 — Chain Rule + FTC
\(\dfrac{d}{dx}\displaystyle\int_0^{x^2} \cos t\,dt\)
FTC + chain rule:
\(= \cos(x^2) \cdot 2x\)
✗ Subtracting in the wrong order
It's always \(F(b) - F(a)\) — upper bound minus lower bound. Writing \(F(a) - F(b)\) flips the sign of the entire answer. Double-check which limit is \(a\) and which is \(b\).
✗ Forgetting the chain rule in FTC Part 1
If the upper limit is \(g(x)\) instead of \(x\), you must multiply by \(g'(x)\). \(\frac{d}{dx}\int_0^{x^2} f(t)\,dt = f(x^2) \cdot 2x\), not just \(f(x^2)\).
✗ Adding +C to a definite integral
The constant \(C\) cancels when you subtract \(F(a)\) from \(F(b)\). You only need \(+C\) for indefinite integrals. Writing \([F(x)+C]_a^b\) is harmless but redundant and confusing.

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