Back to Finding and using Taylor series

Activity 8.5.4

Avg difficulty 2.5

In this activity we will determine the Taylor series expansion for the famous error function, erf⁡(x)=2π∫0xe−t2 dt\begin{gathered} \erf(x) = \frac{2}{\sqrt{\pi}} \int_0^x e^{-t^2} \, dt \end{gathered}, that arises in probability theory and other important applications.

  1. Use the Taylor series for exe^{x} to find the Taylor series for e−t2e^{-t^2}.

  2. Next, evaluate the integral ∫0xe−t2 dt\int_0^x e^{-t^2} \, dt by replacing e−t2e^{-t^2} with its Taylor series.

  3. Use your work in (b) to state the Taylor series for erf⁡(x)=2π∫0xe−t2 dt\erf(x) = \frac{2}{\sqrt{\pi}} \int_0^x e^{-t^2} \, dt

  4. For what interval of xx-values will the Taylor series for erf⁡(x)\erf(x) converge? Why?

  5. In probability theory, erf⁡(x)\erf(x) is important because of its connection to the normal distribution, which is represented by a bell curve. Indeed, erf⁡(x)\erf(x) represents the fraction of a normally distributed characteristic in a population that lies between 00 and xx. How can you use your result in (c) to estimate erf⁡(0.5)\erf(0.5)?

Boelkins, Active Calculus, §8.5 Finding and using Taylor series, Activity 8.5.4

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Adapted from Active Calculus © 2012–2025 Matthew Boelkins. Licensed under CC BY-SA 4.0. Source: Active Calculus. Imported at revision dc86ba3.