So why does the integral represent an infinite sum?

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The integral represents an infinite sum because it is fundamentally based on the concept of Riemann sums, which approximate the area under a curve using the sum of the areas of rectangles. As the number of rectangles increases indefinitely, the Riemann sum converges to the value of the definite integral. The relationship between integrals and derivatives is articulated through the fundamental theorem of calculus, illustrating that integration and differentiation are inverse processes. The discussion also clarifies misconceptions about the Riemann Hypothesis, emphasizing that it pertains to the zeros of the Riemann zeta function and is unrelated to the integral's definition. Thus, the integral's representation as a summation is a core concept in understanding calculus.
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In an earlier post i was shown how to represent an integral as an infinite sum. So why is the anti derivative a summation by definition? For example, the derivative dy/dx is found by f(x+h)-f(x)/h.
 
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lundyjb said:
In an earlier post i was shown how to represent an integral as an infinite sum. So why is the anti derivative a summation by definition? For example, the derivative dy/dx is found by f(x+h)-f(x)/h.

I assume you mean the Riemann integral. Integrals are a sum of infinite rectangles taken over an interval. Each of these rectangles has an area and we use those areas to approximate the integral ( presuming we are talking about definite integrals ).

The Riemann sum, is that sum of the areas of those rectangles, and as we let n→∞ ( we chop the rectangles finely enough so that they cover the area completely ), the sum converges to the same value you will get from the definite integral. Hence why you can write :

##lim_{n→∞} \sum^{n}_{i=0} f(x_{i}^{*}) Δx_i = \int_{a}^{b} f(x) dx##
 
The answer to that question is basically the fundamental theorem of calculus.

To show enough to make this plausible, imagine you break the interval [a,b] into pieces. Call the pieces [a,x1], [x1,x2], [x2,x3] ... [xN-1,xN], [xN,b].
Assume they are equally large intervals and that xi+1-xi=h. Now you have a function F(x) and its derivative is F'(x)=f(x).

To show that the summation definition of the integral is in a sense the opposite of the derivative, we need to show that
\int_{a}^{b}f(x)dx=\int_{a}^{b}F'(x)dx = F(b)-F(a)
Use the definition of the derivative as an approximation (becomes exact as h goes to 0):
F'(x_i)\approx\frac{F(x_{i+1})-F(x_i)}{h}
Now look at the summation definition of the integral (again, only becomes exactly the integral as h goes to 0). Also, for convenience, let a=x0 and b=xN+1.
\int_{a}^{b}F'(x)dx =\sum_{i=0}^{N}F'(x_i)*(x_{i+1}-x_i)
Remember that xi+1-xi=h, so
\int_{a}^{b}F'(x)dx =\sum_{i=0}^{N}F'(x_i)*h
\approx\sum_{i=0}^{N}\frac{F(x_{i+1})-F(x_i)}{h}*h
=\sum_{i=0}^{N}F(x_{i+1})-F(x_i)
This type of sum is called a 'telescoping sum'. Watch what happens when you write the first few terms:
F(x1) -F(x0)+F(x2) -F(x1)+F(x3) -F(x2)+F(x4) -F(x3)
Notice that every term cancels another one except -F(x0) and +F(x4). No matter how many terms you add, all of them will cancel except the first and last. So that integral is
\int_{a}^{b}F'(x)dx = F(x_{N+1})-F(x_0)=F(b)-F(a)

So hopefully that shows how they are opposites.
 
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I thought the 'theoretical' answer to that question was a millenium problem (Riemann Hypothesis). I might be wrong though.
 
CubicFlunky77 said:
I thought the 'theoretical' answer to that question was a millenium problem (Riemann Hypothesis). I might be wrong though.
The Riemann Hypothesis is something else. It relates to the zeroes of the Riemann zeta function. This problem was solved in the 1600's.
 
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