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Section 9.1 Functions defined by integrals

Introduction goes here.
  • One way of defining the natural logarithm is
    \begin{equation*} \ln x=\int_{1}^{x}\frac{1}{t}\dd{t}\text{.} \end{equation*}
    You can then show that this function has all the properties you’d expect of the natural logarithm.
  • Many functions don’t have closed-form antiderivatives! But we do something very similar to deal with them—we define a new function. A few examples:
    • Logarithmic integral:
      \begin{equation*} \mathrm{li}(x)=\int_{0}^{x}\frac{1}{\ln t}\dd{t} \end{equation*}
      This is used in number theory.
    • Fresnel integrals:
      \begin{align*} \mathrm{S}(x) \amp = \int_{0}^{x}\sin(t^{2})\dd{t}\\ \mathrm{C}(x) \amp = \int_{0}^{x}\cos(t^{2})\dd{t} \end{align*}
      These are used in optics. Also there’s lots of cool stuff related to the Euler spiral, parametric stuff from Chapter 6, and a connection to roller coasters!