A definite integral can be defined as the limit as the norm of the partition approaches zero of a function value times a difference in its independent variable. Since I do not have access to a proper symbol library on here, I will try to write it out as best as I can:
lim as p->0 of sum from i=1 to n of f(xi)*(delta-x).
You may know about Riemann sums, which, in functions of one variable, approximate an integral using rectangular partitions of the area under a function's curve that go from the axis in question to some defined value on the curve in height and are some defined width of independent variable.
For instance, to approximate the area between the function y=4-x2 and the x-axis, the following could be done:
Now, that was kind of a long-winded review, but I want to make sure you know that before I continue, and I can refer back to that to simplify my explanation of how limits relate to integrals. As I said above, as the number of partitions you use increases, the approximation of the integral gets more and more accurate. It follows a behavior similar to a limit in that it approaches closer and closer to the actual value of the integral. But, as you increase the number of partitions, the width of the partitions gets smaller and smaller since you are fitting more rectangles into the same space. To get the true value of the integral, you would need an infinite number of zero-width rectangles. This is impossible to definitively calculate, but by taking the limit as the width of the partitions approaches zero, we can find the exact value of the integral.
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Where you refer to a particular integral I will assume you mean a definite integral. To illustrate why there is no constant of integration in the result of a definite integral let me take a simple example. Consider the definite integral of 1 from 0 to 1. The antiderivative of this function is x + C, where C is the so-called constant of integration. Now to evaluate the definite integral we calculate the difference between the value of the antiderivative at the upper limit of integration and the value of it at the lower limit of integration: (1 + C) - (0 + C) = 1 The C's cancel out. Furthermore, they will cancel out no matter what the either antiderivatives happen to be or what the limits of integration happen to be.
This makes it possible to give a precise formal definition of both the derivative, and the definite integral - which are both extremely useful concepts in math, physics, and engineering.
If the upper limit is a function of x and the lower limit is a constant, you can differentiate an integral using the Fudamental Theorem of Calculus. For example you can integrate Integral of [1,x^2] sin(t) dt as: sin(x^2) d/dx (x^2) = sin(x^2) (2x) = 2x sin(x^2) The lower limit of integration is 1 ( a constant). The upper limit of integration is a function of x, here x^2. The function being integrated is sin(t)
First, find the area under the curve y = 1/x2, with boundary lines x = 1 and x = 6, by calculating the integral of 1/x2 with lower limit 1, and upper limit 6. Then divide it by 2. (6)integral(1) of (1/x2) dx = (6)integral(1) of (x--2) dx = -x-1|(6),(1) = -1/x|(6)(1) = -1/6 +1 = 5/6. Thus, the half of the area under the curve is 5/12.
Well, darling, the limit of linearity range is the point at which a linear relationship between two variables breaks down. It's like when your favorite pair of shoes finally give out after miles of walking - they just can't keep up anymore. So, when you hit that limit, you better start looking for a new pair of kicks because things are about to get nonlinear real quick.