FTC Part 1 with Chain Rule
Textbook Reference
| Primary source | OpenStax Calculus Volume 2, Section 1.3: “The Fundamental Theorem of Calculus” |
| Direct link | https://openstax.org/books/calculus-volume-2/pages/1-3-the-fundamental-theorem-of-calculus |
| Original home | OpenStax Calculus Volume 1, Section 5.3: “The Fundamental Theorem of Calculus” |
| Original link | https://openstax.org/books/calculus-volume-1/pages/5-3-the-fundamental-theorem-of-calculus |
| Stewart | Calculus (Stewart), Section 5.3: “The Fundamental Theorem of Calculus” |
This lesson combines FTC Part 1 (from the section above) with the chain rule from differential calculus. The chain rule is in OpenStax Calculus Volume 1, Section 3.6 (https://openstax.org/books/calculus-volume-1/pages/3-6-the-chain-rule). Both sources are free and openly licensed.
When the Upper Limit Is Not Just $x$
In the basic FTC Part 1, the upper limit of integration is simply $x$. But what if the upper limit is something more complicated, like $x^2$ or $\sin x$? You are no longer differentiating with respect to the upper limit directly: you need the chain rule.
This is like reading a speedometer while driving: if the speedometer reading is $v(t)$, and you want to know how fast the reading changes as you accelerate, you need to consider both the speed itself AND how quickly you are changing it. It is a rate of a rate.
Prerequisite Map
Quick Reference
| Property | Value |
|---|---|
| Concept | Fundamental Theorem of Calculus |
| Course | MATH161 (Calculus I) |
| Difficulty | Intermediate |
| Time | ~15 minutes |
Key Concepts
The Formula
If $g(x) = \displaystyle\int_a^{u(x)} f(t)\, dt$, where $u(x)$ is a differentiable function, then:
$$\boxed{g'(x) = f(u(x)) \cdot u'(x)}$$
In Leibniz notation:
$$\frac{d}{dx}\int_a^{u(x)} f(t)\, dt = f(u(x)) \cdot \frac{du}{dx}$$
Why This Works
Think of it as a composition of functions:
- First, FTC1 gives us a function $G(u) = \int_a^u f(t)\, dt$ with $G'(u) = f(u)$
- Then we are computing $g(x) = G(u(x))$
- By the chain rule: $g'(x) = G'(u(x)) \cdot u'(x) = f(u(x)) \cdot u'(x)$
Visualization
┌──────────────┐
x ────► │ u = u(x) │ ────► u
└──────────────┘
│
▼
┌──────────────┐
u ────► │ G(u) = ∫f dt │ ────► G
└──────────────┘
Derivative = f(u(x)) · u'(x)
▲ ▲
│ │
from FTC1 from chain rule
The Pattern to Remember
When differentiating $\displaystyle\int_a^{u(x)} f(t)\, dt$:
- Substitute the upper limit into $f$: write $f(u(x))$
- Multiply by the derivative of the upper limit: $\times\, u'(x)$
Both Limits Variable
For the general case $\displaystyle\int_{v(x)}^{u(x)} f(t)\, dt$, split it:
$$\int_{v(x)}^{u(x)} f(t)\, dt = \int_a^{u(x)} f(t)\, dt - \int_a^{v(x)} f(t)\, dt$$
Then differentiate each piece:
$$\frac{d}{dx}\int_{v(x)}^{u(x)} f(t)\, dt = f(u(x)) \cdot u'(x) - f(v(x)) \cdot v'(x)$$
Practice Problems
Find $\displaystyle\frac{d}{dx}\int_1^{x^2} \cos(t)\, dt$.
Find $h'(x)$ if $h(x) = \displaystyle\int_0^{\sin x} e^{t^2}\, dt$.
Find $\displaystyle\frac{d}{dx}\int_{x^3}^{1} \frac{1}{1+t^4}\, dt$.
Differentiate $g(x) = \displaystyle\int_{\sqrt{x}}^{x^2} \ln(1 + t)\, dt$.
Let $F(x) = \displaystyle\int_\pi^{x^2} \frac{\cos t}{t}\, dt$.
Find the equation of the tangent line to the curve $y = F(x)$ at the point where $x = \sqrt{\pi}$.
Common Misconceptions
differentiating $\int_a^{u(x)} f(t)\,dt$ gives $f(u(x))$ without multiplying by $u'(x)$.
This is the composition-is-not-chaining error. The accumulation function $G(s) = \int_a^s f(t)\,dt$ satisfies $G'(s) = f(s)$ by FTC Part 1. Differentiating $G(u(x))$ with respect to $x$ requires the chain rule: $\frac{d}{dx}G(u(x)) = G'(u(x))\cdot u'(x) = f(u(x))\cdot u'(x)$. For example, $\frac{d}{dx}\int_1^{x^4}\sec t\,dt = \sec(x^4)\cdot 4x^3$, not merely $\sec(x^4)$. Omitting $u'(x)$ is the same oversight as writing $\frac{d}{dx}\sin(x^4) = \cos(x^4)$ instead of $4x^3\cos(x^4)$.
Mastery Checklist
Mental Model
The Odometer Analogy: Imagine $\int_a^{u(x)} f(t)\, dt$ as reading an odometer. If $u(x)$ tells you “how far along the road you are” and $f$ is “the scenery at each point,” then:
- FTC1 says the scenery changes as you move
- The chain rule accounts for how fast you are moving along the road
So the total rate of scenery change = (scenery at current position) × (speed of travel).
Common Mistakes
| Mistake | Correction |
|---|---|
| Forgetting the $u'(x)$ factor | Always multiply by the derivative of the upper limit |
| Sign error when lower limit has $x$ | Flip limits first, then remember the negative sign |
| Evaluating $f$ at $x$ instead of $u(x)$ | Substitute the entire upper limit into $f$ |
Connections
Looking back:
- Basic FTC Part 1 is the special case where $u(x) = x$
- This is a direct application of the chain rule from differentiation
Looking ahead:
- FTC Part 2 shows how to evaluate definite integrals using antiderivatives
- The Leibniz integral rule (later courses) handles even more general cases
Real-world connections:
- In physics: when displacement depends on a function of time in a complicated way
- In economics: when cost depends on production level, which itself depends on time
| Previous | Up | Next |
|---|---|---|
| FTC Part 1 | Skills Index | FTC Part 2 |
Last updated: 2026-01-22