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<record version="17" id="1631">
 <title>antiderivative</title>
 <name>Antiderivative</name>
 <created>2002-02-01 23:52:43</created>
 <modified>2009-03-30 15:54:41</modified>
 <type>Definition</type>
<parent id="11655">fundamental theorem of integral calculus</parent>
 <creator id="17536" name="asteroid"/>
 <author id="17536" name="asteroid"/>
 <author id="2872" name="pahio"/>
 <author id="1863" name="Wkbj79"/>
 <author id="19264" name="hv"/>
 <author id="5079" name="aoh45"/>
 <author id="132" name="xriso"/>
 <classification>
	<category scheme="msc" code="26A36"/>
 </classification>
 <defines>
	<concept>constant of integration</concept>
 </defines>
 <synonyms>
	<synonym concept="antiderivative" alias="general antiderivative"/>
	<synonym concept="antiderivative" alias="indefinite integral"/>
	<synonym concept="antiderivative" alias="primitive"/>
 </synonyms>
 <related>
	<object name="AntiderivativeOfComplexFunction"/>
 </related>
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 <content>Let $I$ be an open interval of $\mathbb{R}$ and\, $f:I \longrightarrow \mathbb{R}$\, a real function.

A function \,$F:I \longrightarrow \mathbb{R}$\, is called an \emph{antiderivative} or a \emph{primitive} of $f$ if $F$ is differentiable and its derivative is equal to $f$, i.e.
\begin{displaymath}
 F'(x) = f(x) \quad \text{for all}\; x \in I.
\end{displaymath}

Note that there are an infinite number of antiderivatives for any function $f$ since any constant can be added or subtracted from any valid antiderivative to yield another equally valid antiderivative.

To account for this, we express the \emph{general antiderivative}, or \emph{indefinite integral}, as follows:
$$ \int f(x)\ dx = F+C$$
where $C$ is an arbitrary constant called the \emph{constant of integration}.  The $dx$ portion means ``with respect to $x$'', because after all, our functions $F$ and $f$ are functions of $x$.\\

There is no loss in generality with this notation since in fact \emph{all} antiderivatives of $f$ take this form as the following theorem demonstrates:\\

{\bf Theorem.}  \emph{Let $F, G$ be two antiderivatives of a given function $f$ defined on an open interval $I$. Then $F-G = \textrm{const}$.}

\emph{Proof.}  Since\, $F'(x) = f(x)$\, and\, $G'(x) = f(x)$,\, we have\, $F'(x)-G'(x) = 0$\, on the whole $I$.\, Thus, by the fundamental theorem of integral calculus,\, $F(x)-G(x) = \textrm{const}$.\, $\square$\\

This is no longer true if the domain of the function $f$ is not an open interval (is not connected).  For that scenario, the following more general result holds:\\

{\bf Theorem.}  \emph{Let $U \subset \mathbb{R}$ be an open set (not necessarily an interval).  Suppose $F, G$ are antiderivatives of a given function $f:U \longrightarrow \mathbb{R}$.  Then $F-G$ is constant in each connected component of $U$ (each interval in $U$).}\\

For example, consider the function \,$f:\mathbb{R}\!\smallsetminus\!\{0\} \longrightarrow \mathbb{R}$\, given by $f(x) = \frac{1}{x}$. Notice that the domain of $f$ is not an interval, but the union of the disjoint intervals \,$(-\infty,\, 0)$\, and \,$(0,\,+\infty)$.  Then, all the antiderivatives of $f$ take the form
\begin{displaymath}
\begin{cases}
\log(-x) + C_1, &amp; $if$\;\; x &lt; 0\\
\log(x) + C_2, &amp; $if$\;\; x &gt; 0
\end{cases}
\end{displaymath}

\subsection{Remarks}
\begin{itemize}
\item For complex functions, the definition of antiderivative is exactly the same and the above results also hold (one just needs to consider ``connected open subsets'' instead of ``open intervals'').
\end{itemize}</content>
</record>
