We begin this chapter with a reminder of a few key concepts from Chapter 5. Let \(f\) be a continuous function on \([a,b]\) which is partitioned into \(n\) equally spaced subintervals as
\begin{equation*}
a\lt x_1 \lt x_2 \lt \cdots \lt x_n\lt x_{n+1}=b.
\end{equation*}
Let \(\dx=(b-a)/n\) denote the length of the subintervals, and let \(c_i\) be any \(x\)-value in the \(i^\text{ th }\) subinterval. Definition 5.3.12 states that the sum
\begin{equation*}
\sum_{i=1}^n f(c_i)\dx
\end{equation*}
is a Riemann Sum. Riemann Sums are often used to approximate some quantity (area, volume, work, pressure, etc.). The approximation becomes exact by taking the limit
\begin{equation*}
\lim_{n\to\infty} \sum_{i=1}^n f(c_i)\dx.
\end{equation*}
Theorem 5.3.20 connects limits of Riemann Sums to definite integrals:
\begin{equation*}
\lim_{n\to\infty} \sum_{i=1}^n f(c_i)\dx = \int_a^b f(x)\ dx.
\end{equation*}
Finally, the Fundamental Theorem of Calculus states how definite integrals can be evaluated using antiderivatives.
This chapter employs the following technique to a variety of applications. Suppose the value \(Q\) of a quantity is to be calculated. We first approximate the value of \(Q\) using a Riemann Sum, then find the exact value via a definite integral. We spell out this technique in the following Key Idea.
This Key Idea will make more sense after we have had a chance to use it several times. We begin with Area Between Curves, which we addressed briefly in Section 5. 5.4.