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Integral calculus theorems

Fundamental Theorem of Calculus Part 1: Derivative of an Integral

FTC part 1: if f is continuous, the derivative of the integral from a to x of f(t) dt is f(x). Statement, graph, chain rule version and worked examples.

Integral calculus theorems Updated 3 min read

At a glance

\frac{d}{dx} \int_a^x f(t)\,dt = f(x)
Hypotheses
f is continuous on [a, b], and F(x) = \int_a^x f(t)\,dt for x in [a, b]
Conclusion
F is continuous on [a, b], differentiable on (a, b), and F'(x) = f(x)
In words
The rate at which accumulated area grows is the height of the curve
Chain rule version
\frac{d}{dx}\int_a^{g(x)} f(t)\,dt = f(g(x))\,g'(x)
Big consequence
Every continuous function has an antiderivative
Course
Calculus 1
On this page
  1. Statement of FTC part 1
  2. What FTC 1 means
  3. Why continuity matters
  4. Worked examples
  5. Common mistakes
  6. Why FTC 1 matters

The fundamental theorem of calculus, part 1 (FTC 1) says that if you build a function by accumulating area under a continuous curve, the derivative of that function is the curve itself. It is the first half of the link between derivatives and integrals.

Statement of FTC part 1

Let f be continuous on [a, b], and define the accumulation function

F(x) = \int_a^x f(t)\,dt, \qquad a \le x \le b

Then F is continuous on [a, b], differentiable on (a, b), and

F'(x) = f(x)

In Leibniz notation, \frac{d}{dx}\int_a^x f(t)\,dt = f(x). The variable t is a dummy variable of integration, and x is the upper limit.

What FTC 1 means

F(x) is the signed area under y = f(t) from a to x. Nudge x a little to the right by h, and the new area is a thin strip of width h and height about f(x). So

\frac{F(x + h) - F(x)}{h} \approx \frac{f(x)\,h}{h} = f(x)

and the approximation becomes exact as h \to 0. The rate at which area accumulates equals the height of the curve.

FTC part 1: area under y = x² from 0 to x grows like F(x) = x³/3
The shaded area up to x = 1.5 is F(1.5) = \frac{1.5^3}{3} = 1.125. The dashed curve F(x) = \frac{x^3}{3} tracks that area, and its slope at each x equals the height x^2.

Why continuity matters

Let f(t) = 0 for t < 0 and f(t) = 1 for t \ge 0, and let F(x) = \int_{-1}^x f(t)\,dt. The accumulated area is

F(x) = \begin{cases} 0 & x < 0 \\ x & x \ge 0 \end{cases}

which has a corner at x = 0. So F'(0) does not exist, and certainly does not equal f(0) = 1. The integral still makes sense, but at the jump the conclusion F' = f fails. Away from the jump, where f is continuous, F' = f still holds.

Worked examples

Example 1: the basic form.

\frac{d}{dx}\int_1^x \sqrt{1 + t^3}\,dt = \sqrt{1 + x^3}

No integration needed, and none possible in elementary terms. Replace t with x and you are done.

Example 2: upper limit is a function of x (chain rule). Find \frac{d}{dx}\int_0^{x^2}\cos t\,dt.

Step 1. Let u = x^2. Then the integral is G(u) = \int_0^u \cos t\,dt, and by FTC 1, G'(u) = \cos u.

Step 2. By the chain rule, \frac{d}{dx}G(x^2) = \cos(x^2)\cdot 2x.

\frac{d}{dx}\int_0^{x^2}\cos t\,dt = 2x\cos(x^2)

Check: the integral equals \sin(x^2), whose derivative is 2x\cos(x^2).

Example 3: both limits depend on x. Find \frac{d}{dx}\int_x^{2x} e^{t^2}\,dt.

Step 1. Split at a constant: \int_x^{2x} = \int_0^{2x} - \int_0^{x}.

Step 2. Differentiate each piece with FTC 1 and the chain rule:

\frac{d}{dx}\int_x^{2x} e^{t^2}\,dt = e^{(2x)^2}\cdot 2 - e^{x^2}\cdot 1 = 2e^{4x^2} - e^{x^2}

Example 4: a lower limit with x. Flip the limits first: \frac{d}{dx}\int_x^5 \sin(t^2)\,dt = \frac{d}{dx}\left(-\int_5^x \sin(t^2)\,dt\right) = -\sin(x^2).

Common mistakes

  1. Forgetting the chain rule factor. \frac{d}{dx}\int_0^{x^2}\cos t\,dt is 2x\cos(x^2), not \cos(x^2).
  2. Plugging in the lower limit too. For \int_a^x f(t)\,dt with constant a, the answer is just f(x). The constant lower limit only shifts F by a constant.
  3. Forgetting the sign when x is in the lower limit. Swapping the limits introduces a minus sign.
  4. Integrating first when it is impossible. Integrands like e^{t^2} have no elementary antiderivative, but FTC 1 still differentiates the integral instantly.

Why FTC 1 matters

FTC 1 proves that every continuous function has an antiderivative, namely \int_a^x f(t)\,dt. That fact is what makes FTC part 2 work, turning definite integrals into simple subtraction. It also defines important functions such as \ln x = \int_1^x \frac{1}{t}\,dt. For the full story of both parts, read the fundamental theorem of calculus guide, and see Riemann sums for the definition of the integral it relies on.

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Frequently asked questions

What does the first fundamental theorem of calculus say?

If f is continuous and F(x) = \int_a^x f(t)\,dt, then F'(x) = f(x). The derivative of the accumulated area function is the original function.

How do you take the derivative of an integral with x in the upper limit?

Replace t in the integrand by the upper limit. If the upper limit is g(x) instead of x, also multiply by g'(x). For example \frac{d}{dx}\int_0^{x^2}\cos t\,dt = 2x\cos(x^2).

What if both limits of integration contain x?

Split the integral at a constant, or use the formula \frac{d}{dx}\int_{h(x)}^{g(x)} f(t)\,dt = f(g(x))\,g'(x) - f(h(x))\,h'(x).

What is the difference between FTC part 1 and part 2?

Part 1 differentiates an integral: \frac{d}{dx}\int_a^x f(t)\,dt = f(x). Part 2 evaluates a definite integral with an antiderivative: \int_a^b f(x)\,dx = F(b) - F(a).

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