MATH 146 – Calculus II
December 1, 2025
Consider a function \(f(x)\) defined on an interval \(a \le t \le b\), and, given a whole number \(n\), divide the interval into \(n\) subintervals of length \(\Delta t = \frac{(b-a)}{n}\) with endpoints \(t_0, t_1, t_2, \dots, , t_n\).
The left (regular) Riemann sum is:
\[ f(t_0) \Delta t + f(t_1) \Delta t + \dots + f(t_{n-1}) \Delta t = \sum_{i=0}^{n-1} f(t_i) \Delta t. \]
Consider a function \(f(x)\) defined on an interval \(a \le t \le b\), and, given a whole number \(n\), divide the interval into \(n\) subintervals of length \(\Delta t = \frac{(b-a)}{n}\) with endpoints \(t_0, t_1, t_2, \dots, , t_n\).
The right (regular) Riemann sum is:
\[ f(t_1) \Delta t + f(t_2) \Delta t + \dots + f(t_n) \Delta t = \sum_{i=1}^{n} f(t_i) \Delta t. \]
Given a continuous function \(f(x)\) on an interval \(a \le t \le b\), the definite integral of \(f(x)\) over \([a,b]\) is the limit:
\[ \begin{aligned} \int_a^b f(t)\,dt &= \lim\limits_{n \to \infty} \sum_{i=1}^{n} f(t_i) \Delta t, & &\text{or} \\ \int_a^b f(t)\,dt &= \lim\limits_{n \to \infty} \sum_{i=0}^{n-1} f(t_i) \Delta t \end{aligned} \]
provided these limits exist. \(f(x)\) is called the integrand and \(a\) and \(b\) are called the limits of integration.
Example: Consider the function \(f(x) = x^2 + 1\) over the interval \([0, 2]\). For a given \(n\), \(\Delta t = \frac{2}{n}\) and \(t_i = \frac{2i}{n}\), so that:
\[ \int_0^2 x^2 + 1 \, dx = \lim\limits_{n \to \infty} ((\frac{2i}{n})^2 + 1) \times (\frac{2}{n}). \]
This sum can be thought of as a sum of areas of rectangles the graph of \(f(x)\).
\[ \int_0^2 x^2 + 1 \, dx = \sum_{i=0}^{4} ((\frac{2i}{5})^2 + 1) \times (\frac{2}{5}) = 4.384 \]
\[ \int_0^2 x^2 + 1 \, dx = \sum_{i=0}^{9} ((\frac{2i}{10})^2 + 1) \times (\frac{2}{10}) = 4.448 \]
\[ \int_0^2 x^2 + 1 \, dx = \sum_{i=0}^{19} ((\frac{2i}{20})^2 + 1) \times (\frac{2}{20}) = 4.571 \]
\[ \int_0^2 x^2 + 1 \, dx = \sum_{i=0}^{49} ((\frac{2i}{50})^2 + 1) \times (\frac{2}{50}) = 4.627264 \]
\[ \int_0^2 x^2 + 1 \, dx = \sum_{i=0}^{99} ((\frac{2i}{100})^2 + 1) \times (\frac{2}{100}) = 4.646808 \]
\[ \int_0^2 x^2 + 1 \, dx = \sum_{i=0}^{999} ((\frac{2i}{1000})^2 + 1) \times (\frac{2}{1000}) = 4.664668 \]
As \(n \to \infty\), this sum becomes the area under the graph of \(f(x)\) over \([a,b]\).
\[ \int_0^2 x^2 + 1 \, dx = \lim\limits_{i \to \infty} \sum_{i=0}^{n-1} ((\frac{2i}{n})^2 + 1) \times (\frac{2}{n}) = \frac{14}{3} \]
Estimates of \(\displaystyle\int_a^b f(x)\,dx\) can be obtained with left sums, right sums, sums from midpoint values of \(f(x)\) or more general types of sums.
In simple cases, the values of \(\displaystyle\int_a^b f(x)\,dx\) can be found simply by finding an area under a graph.
Example: Evaluate \(\displaystyle\int_0^2 -2x + 1\,dx\).
\(\displaystyle\int_a^b f(x)\,dx\) is the signed area – that is, the area between the graph of \(f(x)\) and the \(x\)-axis.
Recall the definition of rate of change: \(r = \dfrac{d}{t}\). This implies that \(d = rt\). Suppose \(v(t)\) is the velocity of an object of an object at time \(t\) and consider the distance traveled over the time interval \(\Delta t\).
\[ \begin{aligned} \int_a^b v(t) \, dt &= \lim\limits_{n \to \infty} \sum_{i = 1}^n v(t_i) \Delta t \\ &= \textrm{distance traveled (displacement)} \\ &= \textrm{area under the graph of } v(t) \end{aligned} \]
The velocity of an object moving along an axis is described by the picture below. Find the displacement of the object from time \(t=0\) to time \(t=4\).
Suppose \(f(t)\) is a continuous function on the interval \([a, b]\) and that \(F(t)\) is an antiderivative of \(f(t)\). Then
\[ \int_a^b f(t) \, dt = F(b) - F(a) \]
Notes:
Example: At 10 a.m. A cistern at a rate of \(R(t) \, \frac{gallons}{hour}\), where \(R(t)\) has the graph given below.
Estimate the amount of water in the tank at noon.
Examples:
Examples:
Note: There is no product or quotient rule for definite integrals.
Every continuous function \(f(x)\) has an antiderivative. If \(f(x)\) is a continuous function on an interval and \(a\) is any point, then the function:
\[ F(x) = \int_a^x f(t) \, dt, \]
is an antiderivative of \(f(x)\). In other words:
\[ \frac{d}{dx} \left[ \int_a^x f(t) \, dt \right] = f(x). \]