The Two Main Antiderivative Rules
Special Case Antiderivatives (The ones you have to memorize)
U-Substitution
Initial Value Problems: Finding the +C
Fundamental Theorem of Calculus Part 1

Fundamental Theorem of Calculus Part 1

The Fundamental Theorem of Calculus Part 1 (FTC1) is not an everyday AP Calculus tool. Meaning you will apply the Fundamental Theorem of Calculus Part 2 on a more regular basis, and use FTC2 frequently in the application of antiderivatives. However, I can guarantee you that you will see the FTC1 included on your AP Calculus in class homework, quizzes, and exams a lot. The reason is that FTC1 is a calculus theorem that involves both a derivative and an antiderivative. It is a very common way to test your understanding of the two concepts, and how they interact with each other.

Definition: Fundamental Theorem of Calculus Part 1 (FTC1)

If you have a continuous function, f , on a closed x-interval [ a , b ], then the antiderivative F ( x ) = a x f ( t ) dt is continuous on [ a , b ]and differentiable on the open interval ( a , b ), and its derivative is f ( x ) , then

F ( x ) = d dx a x f ( t ) dt = f ( x )

Note : The format for applying the FTC1 is very specific. The lower bound, a , on your integral must be a constant , and the upper bound must be an equation, x .

Meaning:

What this rule is saying is that if you have some equation, F ( x ) , that is equal to an integral that fits the specific format requirements,

F ( x ) = a x f ( t ) dt

then when you take the derivative, d dx ,on both sides of the equals (just like you were doing an implicit differentiation problem),

d dx F ( x ) = d dx a x f ( t ) dt

your result will be of the form,

F ( x ) = d dx a x f ( t ) dt = f ( x )

Which is found by plugging your upper bound, x , into the equation, f ( t ) , inside you integral.

Essentially a derivative, d dx , undoes an antiderivative, a x , and the result would be what is inside the integral, f ( t ) , with the upper bound, x , plugged in, f ( x ) .

Simplifying that final step, you see F ( x ) = f ( x ) . This derivative connection is how you will be asked to connect the FTC1 back to local max, local min, intervals of increasing and decreasing.

Note: If your upper bound is more than just an x , you will need do an additional step beyond plugging in the upper bound, you will also need to multiply the f ( x ) by the derivative of the upper bound as well. Just like when you learned derivatives , if that is anything more than just an x , then you are looking at a chain rule derivative , and must multiply by the derivative of the inside piece, DIN .

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