The theorem that ties the whole course together: differentiation and integration are inverse operations. It is what lets us compute integrals without ever returning to sums.
It would be astonishing if two operations invented for unrelated reasons — slopes and areas — turned out to be exact inverses. They do. That is the Fundamental Theorem, and it is why integration becomes "find an antiderivative" instead of summing forever.
Because of it we can solve the differential equations that model nearly everything — orbits, circuits, epidemics (SIR models), and option prices (Black–Scholes). Without it those would be intractable.
Newton's own teacher, Isaac Barrow, glimpsed the connection geometrically; Newton and Leibniz saw it in full. This is the theorem that turned calculus from a collection of tricks into the central tool of science. The name is not an exaggeration.
FTC Part 1 says integration creates an antiderivative. FTC Part 2 says an antiderivative evaluates an integral. Keeping those directions separate prevents most mistakes in this unit.
If $f$ is continuous on $[a,b]$ and $F(x)=\displaystyle\int_a^x f(t)\,dt$, then $F$ is differentiable on $(a,b)$ and $F'(x)=f(x)$. At the endpoints, the corresponding one-sided derivative has the same value.
If $f$ is continuous and $G$ is any antiderivative of $f$ (so $G'=f$), then $$\int_a^b f(x)\,dx=G(b)-G(a).$$
$\displaystyle\int_1^e\frac{\ln x}{x}\,dx$. With $u=\ln x$ an antiderivative is $\tfrac12(\ln x)^2$, so the value is $\tfrac12(1-0)=\tfrac12$.
$\dfrac{d}{dx}\displaystyle\int_{a}^{g(x)}f(t)\,dt=f\!\big(g(x)\big)\,g'(x).$ With both limits variable, differentiate each and subtract.
$\dfrac{d}{dx}\displaystyle\int_{0}^{x^2}\cos t\,dt=\cos(x^2)\cdot2x.$
• In Part 1 the variable is the upper limit; the dummy variable
inside is different ($t$, not $x$).
• With a variable upper limit $g(x)$, don't forget the $g'(x)$ factor.
• Part 2 needs $f$ continuous on $[a,b]$ and an antiderivative $G$ with
$G'=f$ throughout $(a,b)$.
Problems adapted from the MAT137 question bank by Alfonso Gracia-Saz, used under CC BY-SA 4.0. Write full solutions before opening the answer.
Compute $\dfrac{d}{dx}\displaystyle\int_{x}^{3}e^{-t^2}\,dt$.
Evaluate $\displaystyle\int_0^{\pi}\sin x\,dx$.
Find $F'(x)$ if $F(x)=\displaystyle\int_{1}^{x^3}\frac{dt}{1+t^2}$.
If $\displaystyle\int_0^x f(t)\,dt=x\,e^{x}$, find $f$.
Find $F'(x)$ for $F(x)=\displaystyle\int_{2x}^{x^2}\frac{dt}{1+t^2}$.
Evaluate $\displaystyle\int_{\pi/4}^{\pi/3}\sec^2x\,dx$.
Evaluate $\displaystyle\int_0^1\!\left[e^x+e^{-x}-\cos(2x)\right]dx$.
Suppose $f$ is continuous and $\displaystyle\int_0^x e^t f(t)\,dt =\frac{\sin x}{x^2+1}$ for all $x$. Find $f(x)$.
Course coverage. This unit is part of the complete MAT137 topic map. It should cover the following items before you move on:
Use the Alfonso Gracia-Saz MAT137 materials as the primary local spine, with the current UofT single-variable calculus topic split as the completeness check. The added items are original study prompts, not copied textbook exercises.
The spine is: accumulation creates antiderivatives, antiderivatives evaluate accumulation, and the two halves close the loop between differentiation and integration.
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 $F(x)=\int_2^{x^3}\sqrt{1+t^4}\,dt$.
Differentiate $G(x)=\int_x^1 e^{-t^2}\,dt$.
If $v(t)=3t^2$ meters/sec, find displacement from $t=1$ to $t=3$.
Why does FTC Part 1 require continuity in the usual statement?