Properties of the Definite Integral

Read this section to learn about properties of definite integrals and how functions can be defined using definite integrals. Work through practice problems 1-5.

Properties of the Definite Integral

As you read each statement about definite integrals, examine the associated Figure and interpret the property as a statement about areas.

1. \int_{\mathrm{a}}^{\mathrm{a}} \mathrm{f}(x) \mathrm{d} \mathrm{x}=0                                    (a definition)

2. \int_{b}^{a} f(x) d x=-\int_{a}^{b} f(x) d x               (a definition)

3. \int_{a}^{b} k d x=k \cdot(b-a)                          (Fig. 1)

4.  \int_{a}^{b} k \cdot f(x) d x=k \cdot \int_{a}^{b} f(x) d x

5. \int_{a}^{b} f(x) d x+\int_{b}^{c} f(x) \mathrm{dx}=\int_{b}^{c} \mathrm{f}(x) \mathrm{d} x              (Fig. 2)


Justification of Property 3: Using area: If k>0 then \int_{\mathrm{a}}^{\mathrm{b}} \mathrm{k} \mathrm{dx} represents the area of the rectangle with base = b–a and height = k, so \int_{\mathrm{a}}^{\mathrm{b}} \mathrm{k} \mathrm{d}
    \mathrm{x}=(\text { height }) \cdot(\text { base })=\mathrm{k}\cdot(\mathrm{~b}-\mathrm{a})


Using Riemann Sums: For every partition \mathrm{P}=\left\{x_{0}=\mathrm{a}, x_{1}, x_{2}, x_{3}, \ldots, x_{\mathrm{n}-1}, x_{\mathrm{n}}=\mathrm{b}\right\} of the interval [a, b], and every choice of \mathrm{c}_{\mathrm{k}}, the Riemann sum is

\begin{aligned} \sum_{k=1}^{n} f\left(c_{k}\right) \cdot \Delta x_{k} &=\sum_{k=1}^{n} \mathrm{k} \cdot \Delta x_{k}=k \sum_{k=1}^{n} \Delta x_{k} \\ &=k \sum_{k=1}^{n}\left(x_{k}-x_{k-1}\right)=k\left\{\left(x_{1}-x_{0}\right)+\left(x_{2}-x_{1}\right)+\left(x_{3}-x_{2}\right)+\ldots+\left(x_{n-1}-x_{n}\right)\right\}
    \\ &=k \cdot\left(x_{n}-x_{0}\right)=k \cdot(b-a) \end{aligned}

so the limit of the Riemann sums, as the mesh approaches zero, is \mathrm{k} \cdot(\mathrm{b}-\mathrm{a}) . \int_{\mathrm{a}}^{\mathrm{b}} \mathrm{k} \mathrm{d} x=\mathrm{k} \cdot(\mathrm{b}-\mathrm{a}).


Justification of Property 4:

\int_{\mathrm{a}}^{\mathrm{b}} \mathrm{k} \cdot \mathrm{f}(x) \mathrm{dx}=\lim _{\operatorname{mesh} \varnothing 0}\left(\sum_{\mathrm{k}=1}^{\mathrm{n}} \mathrm{k} \cdot \mathrm{f}\left(\mathrm{c}_{\mathrm{k}}\right) \Delta \mathrm{x}_{\mathrm{k}}\right)=\mathrm{k}
    \cdot \lim _{\operatorname{mesh} \varnothing 0}\left(\sum_{\mathrm{k}=1}^{\mathrm{n}} \mathrm{f}\left(\mathrm{c}_{\mathrm{k}}\right) \Delta \mathrm{x}_{\mathrm{k}}\right)=\mathrm{k} \cdot \int_{\mathrm{a}}^{\mathrm{b}} \mathrm{f}(x) \mathrm{dx} .

Property 5 can be justified using Riemann sums, but Fig. 2 graphically illustrates why it is true.