Differentiation and integration are inverse operations — proved here from the Riemann definition, using the EVT for Part 1 and the Mean Value Theorem for Part 2. Everything built since Unit 2 comes together on this page.
Two operations invented for unrelated reasons — slopes and areas — turn out to be exact inverses. That is what lets us integrate by finding antiderivatives instead of summing forever.
It is what makes differential equations solvable — the models behind orbits, circuits, epidemics, and the Black–Scholes option price all rely on it.
Newton's teacher Isaac Barrow glimpsed the link geometrically; Newton and Leibniz saw it in full. This is the result that turned calculus from a bag of tricks into the central tool of science.
Let $f$ be integrable on $[a,b]$ and $F(x)=\displaystyle\int_a^x f$. If $f$ is continuous at $x$, then $F$ is differentiable at $x$ and $F'(x)=f(x)$.
If $f$ is integrable on $[a,b]$ and $G$ is an antiderivative of $f$ on $[a,b]$ (meaning $G'=f$ there), then $$\int_a^b f=G(b)-G(a).$$
$\displaystyle\int_1^e\frac{\ln x}{x}\,dx$: an antiderivative of $\tfrac{\ln x}{x}$ is $\tfrac12(\ln x)^2$ (check by the chain rule), so the value is $\tfrac12(1^2-0^2)=\tfrac12$.
For continuous $f$ and differentiable $g$, $\dfrac{d}{dx}\displaystyle\int_a^{g(x)}f(t)\,dt=f\big(g(x)\big)\,g'(x)$ — Part 1 composed with the chain rule. With both limits variable, differentiate each and subtract.
$\dfrac{d}{dx}\displaystyle\int_0^{x^2}\cos t\,dt=\cos(x^2)\cdot2x$ — and you can confirm it by evaluating the integral to $\sin(x^2)$ first.
• In Part 1 the variable is the upper limit; the dummy variable inside is a
different letter.
• With a variable upper limit $g(x)$, keep the $g'(x)$ factor.
• Part 2 needs $G'=f$ on the whole interval — an antiderivative that misses
one point can change the game (corners in $F$ at jumps of $f$).
• Part 1 at a discontinuity of $f$ can fail: $F$ need not be differentiable
there.
Original problems written for this guide in the style of Spivak's exercises. Write a full solution before opening the answer.
Compute $\dfrac{d}{dx}\displaystyle\int_0^{x^2}\cos t\,dt$.
Evaluate $\displaystyle\int_1^e\dfrac{\ln x}{x}\,dx$.
If $f$ is continuous and $\displaystyle\int_0^x f=x e^x$ for all $x$, find $f$.
Find $F'(x)$ for $F(x)=\displaystyle\int_x^{2x}e^{-t^2}\,dt$.
Suppose $f$ is continuous and $\displaystyle\int_0^x f=\int_x^1 f$ for every $x\in[0,1]$. Prove $f\equiv0$.
Evaluate $\displaystyle\int_0^{\pi}\sin x\,dx$.
Compute $\dfrac{d}{dx}\displaystyle\int_{\sin x}^{1}\sqrt{1+t^2}\,dt$.
Let $f$ be continuous on $[a,b]$ and $F(x)=\int_a^x f$. Prove there is $M$ with $|F(x)-F(y)|\le M|x-y|$ for all $x,y\in[a,b]$.
Course coverage. This unit is part of the complete MAT158H1 topic map. It should cover the following items before you move on:
Use the current UofT MAT158H1 calendar topics as the coverage spine, and pair lecture notes with a Spivak-style proof-calculus text for extra reading. The exact assigned textbook should still be checked against the instructor syllabus.
The FTC spine is: continuity gives differentiable accumulation; any antiderivative differs by a constant; definite integrals become endpoint differences.
Use these after the main practice set. They are designed to force definition-level reasoning, theorem selection, and mixed application rather than routine calculation only.
Differentiate $F(x)=\int_a^x f(t)dt$ when $f$ is continuous.
If $G\prime=f$, prove $\int_a^b f=G(b)-G(a)$.
Differentiate $\int_0^{x^2}\cos(t^3)dt$.
Explain substitution for definite integrals as an FTC result.