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6.4 - The Fundamental Theorem of Calculus and Accumulation Functions

Review: The Definite Integral

The definite integral is the area under the curve on a specific interval:
∫abf(x) dx\int_a^b f(x) \, dx
  • aa is the lower limit (a constant)
  • bb is the upper limit (a constant)
  • The result is a number, the total area

Accumulation Functions

An accumulation function has a variable as its upper limit:
F(x)=∫axf(t) dt\boxed{F(x) = \int_a^x f(t) \, dt}
Key points: - The lower limit aa is a constant - The upper limit xx is a variable - We use a different variable (tt) inside to avoid confusion - F(x)F(x) is a function that depends on where we stop - As xx changes, the area accumulates
Why different variables? Because xx is already being used as the upper limit. The tt is a “dummy variable,” and it could be any letter except xx.

Example: Building an Accumulation Function

Given a piecewise linear function f(t)f(t) on [0,5][0, 5]:
6.4 - The Fundamental Theorem of Calculus and Accumulation Functions
Define F(x)=∫0xf(t) dtF(x) = \int_0^x f(t) \, dt and accumulate the area:
xx
F(x)=∫0xf(t) dtF(x) = \int_0^x f(t) \, dt
Calculation
0
0
No area from 0 to 0
1
2.5
Area from 0 to 1
2
4
Previous (2.5) + new area (1.5)
3
5
Previous (4) + new area (1)
4
5.5
Previous (5) + new area (0.5)
5
5
Previous (5.5) − area below the axis (0.5)
6.4 - The Fundamental Theorem of Calculus and Accumulation Functions
F(x)F(x) shows the total accumulated area from t=0t = 0 to t=xt = x.
Integrals can define new functions. Some functions can’t be written with powers, roots, trig, exponentials, or logs at all. For example:
S(x)=∫0xsin⁡(t2) dtS(x) = \int_0^x \sin(t^2) \, dt
There’s no algebra formula for S(x)S(x), but it’s still a perfectly good function. Every xx gives one value (the net area from 0 to xx), so you can graph it, evaluate it with a calculator, and find its derivative with the theorem below: S′(x)=sin⁡(x2)S'(x) = \sin(x^2).

The Fundamental Theorem of Calculus (Part 2)

ddx[∫axf(t) dt]=f(x)\boxed{\frac{d}{dx}\left[\int_a^x f(t) \, dt\right] = f(x)}
In words: the derivative of an integral gives you back the original function.
Condition: this works when ff is continuous on an interval that contains aa, for any xx in that interval.
The big idea here is that derivatives and integrals are inverse operations. They undo each other, the same way division undoes multiplication.
Terminology
If F(x)=∫axf(t) dtF(x) = \int_a^x f(t) \, dt, then: - F(x)F(x) is an antiderivative of f(x)f(x) - f(x)f(x) is the integrand (what’s inside the integral) - Integral of ff = antiderivative = FF - Derivative of FF = original function = ff
If F(x)=∫f(x) dx, then F′(x)=f(x)\text{If } F(x) = \int f(x) \, dx \text{, then } F'(x) = f(x)

Applying the Theorem

Basic case: constant lower limit
Given F(x)=∫2x(3t2+4t) dtF(x) = \int_2^x (3t^2 + 4t) \, dt, find F′(x)F'(x).
Just plug in xx for tt:
F′(x)=3x2+4xF'(x) = 3x^2 + 4x
Steps: 1. Recognize the constant lower limit (2) 2. Variable upper limit (xx) 3. Replace tt with xx in the integrand 4. Done
With the chain rule: upper limit is a function
Given F(x)=∫ag(x)f(t) dtF(x) = \int_a^{g(x)} f(t) \, dt:
F′(x)=f(g(x))⋅g′(x)\boxed{F'(x) = f(g(x)) \cdot g'(x)}
Steps: 1. Plug g(x)g(x) in for tt in the integrand 2. Multiply by the derivative of g(x)g(x)
Example 1
Given F(x)=∫1x3sin⁡(t) dtF(x) = \int_1^{x^3} \sin(t) \, dt, find F′(x)F'(x).
F′(x)=sin⁡(x3)⋅ddx[x3]=sin⁡(x3)⋅3x2=3x2sin⁡(x3)F'(x) = \sin(x^3) \cdot \frac{d}{dx}[x^3] = \sin(x^3) \cdot 3x^2 = 3x^2 \sin(x^3)
Example 2
Given F(x)=∫04xh(t) dtF(x) = \int_0^{4x} h(t) \, dt, find F′(x)F'(x).
F′(x)=h(4x)⋅ddx[4x]=4h(4x)F'(x) = h(4x) \cdot \frac{d}{dx}[4x] = 4h(4x)
Notice we never needed to know what h(t)h(t) actually is. Just plug in and apply the chain rule.

Both Limits Are Functions

Given F(x)=∫h(x)g(x)f(t) dtF(x) = \int_{h(x)}^{g(x)} f(t) \, dt:
F′(x)=f(g(x))⋅g′(x)−f(h(x))⋅h′(x)\boxed{F'(x) = f(g(x)) \cdot g'(x) - f(h(x)) \cdot h'(x)}
Steps: 1. Upper limit: plug in g(x)g(x), multiply by g′(x)g'(x) 2. Subtract 3. Lower limit: plug in h(x)h(x), multiply by h′(x)h'(x)
Mnemonic: “top minus bottom.”
Example 3
Given F(x)=∫−xx5t dtF(x) = \int_{-x}^{x} 5t \, dt, find F′(x)F'(x).
Upper limit contribution:
5(x)⋅ddx[x]=5x⋅1=5x5(x) \cdot \frac{d}{dx}[x] = 5x \cdot 1 = 5x
Lower limit contribution:
5(−x)⋅ddx[−x]=(−5x)(−1)=5x5(-x) \cdot \frac{d}{dx}[-x] = (-5x)(-1) = 5x
Combine (top minus bottom):
F′(x)=5x−5x=0F'(x) = 5x - 5x = 0
Why zero? The integral is symmetric about the origin, so the accumulated value never changes.
Example 4
Given F(x)=∫2x3x(t2−t) dtF(x) = \int_{2x}^{3x} (t^2 - t) \, dt, find F′(x)F'(x).
Upper limit (3x3x): - Plug in: (3x)2−(3x)=9x2−3x(3x)^2 - (3x) = 9x^2 - 3x - Chain rule: multiply by 3 - Result: 27x2−9x27x^2 - 9x
Lower limit (2x2x): - Plug in: (2x)2−(2x)=4x2−2x(2x)^2 - (2x) = 4x^2 - 2x - Chain rule: multiply by 2 - Result: 8x2−4x8x^2 - 4x
Subtract lower from upper:
F′(x)=(27x2−9x)−(8x2−4x)=19x2−5xF'(x) = (27x^2 - 9x) - (8x^2 - 4x) = 19x^2 - 5x

Summary of Cases

Type
Formula
Notes
Constant lower, variable upper
ddx[∫axf(t) dt]=f(x)\frac{d}{dx}\left[\int_a^x f(t) \, dt\right] = f(x)
Just plug in xx
Constant lower, function upper
ddx[∫ag(x)f(t) dt]=f(g(x))⋅g′(x)\frac{d}{dx}\left[\int_a^{g(x)} f(t) \, dt\right] = f(g(x)) \cdot g'(x)
Use the chain rule
Both variable
ddx[∫h(x)g(x)f(t) dt]=f(g(x))⋅g′(x)−f(h(x))⋅h′(x)\frac{d}{dx}\left[\int_{h(x)}^{g(x)} f(t) \, dt\right] = f(g(x)) \cdot g'(x) - f(h(x)) \cdot h'(x)
Top minus bottom

Common Mistakes to Avoid

  • Forgetting the chain rule when the upper or lower limit isn’t just xx
  • Using the same variable inside and outside. Don’t write ∫axf(x) dx\int_a^x f(x) \, dx; use a different variable inside
  • Sign error with the lower limit. You SUBTRACT the lower limit contribution, you don’t add it
  • Not applying the derivative to the limits. You have to multiply by g′(x)g'(x) or h′(x)h'(x)

Key Takeaways

  • Accumulation function: F(x)=∫axf(t) dtF(x) = \int_a^x f(t) \, dt accumulates area as xx varies
  • FTC Part 2: ddx[∫axf(t) dt]=f(x)\frac{d}{dx}\left[\int_a^x f(t) \, dt\right] = f(x), so the derivative undoes the integral
  • Antiderivative: the integral of ff gives an antiderivative FF where F′=fF' = f
  • Basic case: constant lower limit means you just plug in the upper limit
  • Chain rule: when the upper limit is g(x)g(x), multiply by g′(x)g'(x)
  • Both limits variable: top contribution MINUS bottom contribution
  • Different variables: use tt (or another letter) inside the integral, save xx for the limit
  • Derivatives and integrals are inverses: they cancel each other out
  • This theorem is genuinely fundamental. It’s the bridge between differentiation and integration

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