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<record version="3" id="3342">
 <title>universal relation</title>
 <name>UniversalFormula</name>
 <created>2002-08-23 21:00:08</created>
 <modified>2002-08-24 13:40:42</modified>
 <type>Definition</type>
 <creator id="455" name="Henry"/>
 <author id="455" name="Henry"/>
 <classification>
	<category scheme="msc" code="03B10"/>
 </classification>
 <defines>
	<concept>universal function</concept>
 </defines>
 <synonyms>
	<synonym concept="universal relation" alias="universal"/>
 </synonyms>
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 <content>If $\Phi$ is a class of $n$-ary relations with $\vec{x}$ as the only free variables, an $n+1$-ary formula $\psi$ is \emph{universal} for $\Phi$ if for any $\phi\in\Phi$ there is some $e$ such that $\psi(e,\vec{x})\leftrightarrow\phi(\vec{x})$. In other words, $\psi$ can simulate any element of $\Phi$.

Similarly, if $\Phi$ is a class of function of $\vec{x}$, a formula $\psi$ is universal for $\Phi$ if for any $\phi\in\Phi$ there is some $e$ such that $\psi(e,\vec{x})=\phi(\vec{x})$.</content>
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