G.MATH
CALCULUS
The Fundamental Theorem of Calculus

It's a pity that most students studying Calculus take the definite integral for granted. I notice that many of them blindly substitute the limits of integral when finding areas without knowing the processes which are at work to make the substitution possible.

In this section, I will explain to the best as I can the Fundamental Theorem of Calculus, the reason why we can so easily find the areas under the graph.
VIDEO LECTURE part 2


MAIN CONCEPTS
where is any antiderivative of .
Get the Printer Friendly Version
COMMENTS
Feel free to leave any comments on the lesson - your views, improvements, mistakes, clarification of concepts, or vote to have this lesson revised.

LESSON
All high school calculus courses will most probably start a discussion on the integral calculus with the Riemann sums. While it does work by taking the sum of small little areas below the graph, we get a rather complicated definition of the definite integral as

While this method does work, it is impractical and in some case even impossible to use when evaluating complicated integrals such as

 and

Thus begs the question, how do we progress in evaluating these integrals, and in turn finding the area under the graph, bearing in mind that they didn’t have calculators in those days. Nonetheless, from the mind of Newton and Leibniz came a new method.

Their method of calculating the definite integral of such functions seems paradoxical in first sight. The approach was to ask a more difficult question: Instead of considering a fixed area like the graph on the left, how do we calculate the variable area, denoted by , when the right side of the area is considered movable. 

The objective here is to find  where the area is a function of . Clearly  and  is the fixed area in the graph on the left. We need to find an explicit formula for  and then determine the area by letting . This is a two-step process. You ready? Then let’s go!

Step 1. We need to establish the fact that

which says that the rate of change of area  with respect to a change in  is equal to the length to the right of the region, or equivalently . Well this may or may not be obvious we shall prove it here. Recall differentiating by first principles,

Now  is the area under the graph from  to  and  is the area between  and . And thus the expression  is the area between  and . By the mean value theorem, we see that this area is exactly equal to the area of a rectangle with the same base whose height is  where  lies between  and .


 

Using the graphical reasoning above, we can write

since  is continuous. For further elaboration,  is equivalent to . Since  is caught between  and , we also have , and in turn .

Step 2. In the previous step, we have the equation

This allows us to find a formula for the area . Now,  is one of the antiderivatives of . I emphasize ONE of the antiderivatives because we know from differentiating that is that we can differentiate a any constant and get the same result. So now say that  is any antiderivative of  and thus

To determine , we let  knowing that this will give us  and so . Therefore

Reintroducing the point  as we have shown on the graph, recognize that

And so I present to you the Fundamental Theorem of Calculus:

If  is continuous on a closed interval , and if  is any antiderivative of  so that , then

Out of convenience and convention, we can also write

though I must stress that this actually means from the antiderivative of . We can now reduce the problem of evaluating definite integrals of complicating functions to finding their antiderivatives.

All information presentated, less questions and exercises, is original content of Donny, with slight references to various books.
Video courtesy of YouTube.com service.
gtech gmech gphys