Connection between differentiation and integration.
Deep-dive lesson - accessible entry point but dense material. Use worked examples and spaced repetition.
You already know two powerful calculus tools: derivatives (instantaneous rate of change) and definite integrals (accumulated area). The Fundamental Theorem of Calculus (FTC) is the bridge that explains why these two ideas are secretly the same process viewed from opposite directions.
FTC has two linked parts: (1) If you build an “accumulation function” F(x) = ∫ₐˣ f(t) dt, then F′(x) = f(x). (2) If F is any antiderivative of f, then ∫ₐᵇ f(x) dx = F(b) − F(a). Together they turn hard area problems into endpoint subtraction and explain why antiderivatives matter.
Before FTC, you might experience calculus as two separate worlds:
FTC answers a natural question:
If integration is “adding up tiny pieces,” and differentiation measures the “instantaneous change,” are these operations related?
They are related in the strongest possible way: integration and differentiation are inverse processes (up to a constant).
FTC is commonly presented in two parts.
Let be continuous on an interval containing . Define an accumulation function
Then
Interpretation: If $F(x)$ measures “area accumulated up to $x$,” then the rate at which that area grows at position $x$ equals the height of the curve there.
If is continuous on and is any antiderivative of (meaning ), then
Interpretation: Net accumulated change equals the antiderivative’s endpoint difference.
Imagine the interactive canvas shows the curve , a fixed vertical line at , and a movable vertical line at .
As you drag to the right, you shade the region under from to . The shaded area is .
Canvas state mapping:
The key claim of Part 1 is that the slope of the traced $F$ graph at the current $x$ equals the current height $f(x)$.
That is the heart of FTC: slope-of-area equals height-of-curve.
Think of as “net area accumulated.”
If you increase by a tiny amount , you add a thin vertical slice of area from to .
If is very small, that slice’s area is approximately a rectangle:
So the added area is approximately .
But the added area is also exactly .
So we expect
which implies
Taking the limit as gives .
Use this mental picture even without the canvas.
y
^
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| /\
| / \ curve y=f(x)
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|_______/______\____________> x
a x x+h
Shaded area from a to x is F(x)
Thin slice from x to x+h has area ≈ f(x)·hCanvas tie-in: In an interactive version, the thin slice is the last sliver of shaded region as you nudge to .
Start with
Compute the difference:
Now form the difference quotient:
If is continuous, then on the tiny interval , is close to .
A standard argument (using the Mean Value Theorem for Integrals) says there exists some such that
So
As , the point , and by continuity . Therefore
It says something precise:
If you define as the integral from a constant up to the variable endpoint , then differentiating returns the original integrand.
When you see
read it as: “ is a function whose input is the upper limit.”
So has its own graph, its own slope, and its own values.
In the interactive canvas, you can imagine two linked plots:
FTC Part 1 is the rule that synchronizes these plots: the slope on Plot 2 equals the height on Plot 1.
Definite integrals look like they should require adding infinitely many tiny rectangles.
But in practice, we almost never compute them that way.
FTC Part 2 is the practical miracle:
If you can find any antiderivative of , then the definite integral is just .
This turns an accumulation problem into an endpoint subtraction problem.
Part 1 gives you a way to create an antiderivative.
Define
Then Part 1 says . So is an antiderivative of .
Now evaluate at :
Also, .
So
But any two antiderivatives differ by a constant. If , then .
So
That’s Part 2.
Think of as a height function whose change equals area under .
F(x)
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| • (b, F(b))
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| • (a, F(a))
+----------------------------> x
a b
Vertical change: F(b)-F(a)
Equals signed area under f from a to b.Canvas tie-in: Imagine toggling a mode where instead of shading area under , you watch a point move on the graph of an antiderivative . The theorem says the vertical difference between the endpoint values equals the shaded area you would have gotten.
Remember the definite integral is signed:
FTC Part 2 preserves that: if is negative on much of , then will reflect a net decrease.
Also note the direction:
That matches the endpoint rule:
FTC Part 2 gives a recipe:
This is why learning antiderivative patterns (power rule, trig, substitution later) is so valuable.
| Idea | Input | Output | Typical use |
|---|---|---|---|
| FTC Part 1 | A definite integral with variable top: | A derivative: | Differentiate an accumulation function |
| FTC Part 2 | A function and bounds | A number | Compute a definite integral via antiderivative |
Suppose is a rate:
Then the accumulated total from to is
FTC Part 2 says you can compute that total if you can find an antiderivative.
This is FTC Part 1 in words:
If is total accumulated amount up to time , then is the instantaneous rate at time .
So FTC explains why “total” and “rate” are inverse ideas:
Often you’ll see a function defined by an integral that you cannot evaluate in elementary terms, like
Even if you can’t find a closed-form antiderivative, FTC Part 1 still gives
That’s extremely useful for analyzing monotonicity, slopes, and local behavior.
If the canvas had three layers:
Then moving produces two simultaneous changes:
FTC Part 1 says: the instantaneous rise-per-run of that point equals the current function height.
Indefinite integrals represent families of antiderivatives:
FTC Part 2 avoids worrying about because subtraction cancels it:
So definite integrals are often cleaner than indefinite integrals: the constant disappears automatically.
FTC is a hub concept:
If you keep one sentence in mind, make it this:
Net accumulation over an interval equals antiderivative change across the endpoints.
Let
Find F′(x).
Recognize the structure: F(x) is defined as an integral with variable upper limit x.
So FTC Part 1 applies directly: if F(x)=∫ₐˣ f(t)dt, then F′(x)=f(x).
Identify the integrand as f(t)=3t²−4t+1.
FTC Part 1 says:
Compute:
Insight: You don’t need to evaluate the integral first. The derivative of “area up to x” is just the curve height at x.
Compute
Find an antiderivative F of f(x)=2x−5.
Use basic rules:
∫2x dx = x², and ∫(−5) dx = −5x.
So one antiderivative is
Apply FTC Part 2:
Evaluate endpoints:
Subtract:
Insight: The result is negative because (2x−5) is below the x-axis on much of [1,3]. FTC preserves signed area automatically.
Let
Find H′(x).
Notice the upper limit is not x but x². We’ll combine FTC Part 1 with the chain rule.
Let G(u)=∫₀ᵘ sin(t) dt. Then by FTC Part 1:
Now H(x)=G(x²). Differentiate using the chain rule:
Substitute G′(x²)=sin(x²) and d/dx(x²)=2x:
Insight: FTC Part 1 tells you the derivative with respect to the upper limit; the chain rule accounts for how the upper limit depends on x.
FTC connects differentiation and integration as inverse processes (up to a constant).
FTC Part 1: If F(x)=∫ₐˣ f(t)dt, then F′(x)=f(x) (slope of accumulated area equals curve height).
FTC Part 2: If F′=f, then ∫ₐᵇ f(x)dx = F(b)−F(a) (definite integrals become endpoint subtraction).
The “thin slice” view explains Part 1: increasing x by h adds an area ≈ f(x)·h.
Definite integrals are signed; negative results correspond to net area below the x-axis.
You can differentiate many integral-defined functions even when the integral has no elementary closed form.
The constant of integration cancels in F(b)−F(a), which is why definite integrals are often simpler than indefinite ones.
Treating ∫ₐˣ f(t)dt as if it were an indefinite integral and forgetting it defines a new function of x.
Forgetting that FTC Part 1 returns f(x), not the antiderivative of f.
Dropping the chain rule when the upper limit is something like x² or 3x+1.
Confusing signed area with geometric area (expecting a nonnegative answer even when f is negative).
Let F(x)=∫₋1ˣ (t³+2) dt. Compute F′(x).
Hint: FTC Part 1: derivative of integral from a to x is the integrand evaluated at x.
Here f(t)=t³+2, so by FTC Part 1:
Compute the definite integral ∫₀² (x² − 4x) dx using FTC Part 2.
Hint: Find an antiderivative: ∫x² dx = x³/3 and ∫(−4x) dx = −2x².
An antiderivative is
Then
Compute:
So the integral is .
Let H(x)=∫₁^{3x} \sqrt{1+t} \,dt. Find H′(x).
Hint: Think of H(x)=G(3x) where G(u)=∫₁ᵘ √(1+t) dt. Apply FTC Part 1 then chain rule.
Define
By FTC Part 1:
Now , so