Consider the function:
\[ f(x) = x^2 \]
The process of integration for this function starts in the form of adding the areas of many rectangles via a Riemann sum. The heights of these rectangles are determined by the value of the function at the relevant x value, and the width is decided by the amount of partitions over the bounds of integration. The process of integration sums up the area of infinitely thin rectangles over the relevant bounds. In this case there is a function of one variable over a domain in \( \mathbb{R} \). Now consider the function:
\[ f(x,y) = x^2 + y^2 \]
Now we have a function of 2 variables. An integral for this function can now be integrated over \(\mathbb{R}^2\), which can be viewed as an area rather than a line in \( \mathbb{R}\). The other major difference for integration over a two dimensional domain is having two variables to integrate. This means that the integral is taking with respect to an area or \( dA \). For this integral, the Riemann sum consists of rectangular prisms as opposed to rectangles. Their heights are still defined by the function, and their widths and lengths are defined by the number of partitions over the domain. For an integration with respect to \( dA \), the rectangular prisms have two dimensions that are infinitely small, and the sum of the volume of these skinny prisms is equivalent to the integral of the function with respect to the domain.
Most math teachers I've had have been able to break down Calculus into two very broad categories: derivatives and integrals. What is truly amazing, is how much you can do with these two tools. By using integration, it is possible to approximate the shape of a 2-D function that is rotated around an axis. This solid created from the rotation is known as a solid of revolution. To explain this concept, we will take a look at the region bounded by the two functions: \[ f(x) = 2^{.25x} - 1 \] and \[ g(x) = e^{.25x} - 1 \] bounded at the line y = 1. This region is meant to represent a cross section of a small bowl. While it may not perfectly represent this practical object, the approximation will be quite textured, and will provide insight into how the process works. The region bounded by the two functions can be rotated around the y-axis to create a fully solid object. This is easy enough to talk about, but what exactly does this new solid look like? Is...


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