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	<id>https://rigidgeometricalgebra.org/wiki/index.php?action=history&amp;feed=atom&amp;title=Commutators</id>
	<title>Commutators - Revision history</title>
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	<updated>2026-04-16T23:08:21Z</updated>
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		<id>https://rigidgeometricalgebra.org/wiki/index.php?title=Commutators&amp;diff=84&amp;oldid=prev</id>
		<title>Eric Lengyel: Created page with &quot;In geometric algebra, there are four ''commutator'' products defined as follows.  :$$[\mathbf a, \mathbf b]^{\Large\unicode{x27D1}}_- = \dfrac{1}{2}\left(\mathbf a \mathbin{\unicode{x27D1}} \mathbf b - \mathbf b \mathbin{\unicode{x27D1}} \mathbf a\right)$$  :$$[\mathbf a, \mathbf b]^{\Large\unicode{x27D1}}_+ = \dfrac{1}{2}\left(\mathbf a \mathbin{\unicode{x27D1}} \mathbf b + \mathbf b \mathbin{\unicode{x27D1}} \mathbf a\right)$$  :$$[\mathbf a, \mathbf b]^{\Large\unicode...&quot;</title>
		<link rel="alternate" type="text/html" href="https://rigidgeometricalgebra.org/wiki/index.php?title=Commutators&amp;diff=84&amp;oldid=prev"/>
		<updated>2023-07-15T06:36:24Z</updated>

		<summary type="html">&lt;p&gt;Created page with &amp;quot;In geometric algebra, there are four &amp;#039;&amp;#039;commutator&amp;#039;&amp;#039; products defined as follows.  :$$[\mathbf a, \mathbf b]^{\Large\unicode{x27D1}}_- = \dfrac{1}{2}\left(\mathbf a \mathbin{\unicode{x27D1}} \mathbf b - \mathbf b \mathbin{\unicode{x27D1}} \mathbf a\right)$$  :$$[\mathbf a, \mathbf b]^{\Large\unicode{x27D1}}_+ = \dfrac{1}{2}\left(\mathbf a \mathbin{\unicode{x27D1}} \mathbf b + \mathbf b \mathbin{\unicode{x27D1}} \mathbf a\right)$$  :$$[\mathbf a, \mathbf b]^{\Large\unicode...&amp;quot;&lt;/p&gt;
&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;In geometric algebra, there are four ''commutator'' products defined as follows.&lt;br /&gt;
&lt;br /&gt;
:$$[\mathbf a, \mathbf b]^{\Large\unicode{x27D1}}_- = \dfrac{1}{2}\left(\mathbf a \mathbin{\unicode{x27D1}} \mathbf b - \mathbf b \mathbin{\unicode{x27D1}} \mathbf a\right)$$&lt;br /&gt;
&lt;br /&gt;
:$$[\mathbf a, \mathbf b]^{\Large\unicode{x27D1}}_+ = \dfrac{1}{2}\left(\mathbf a \mathbin{\unicode{x27D1}} \mathbf b + \mathbf b \mathbin{\unicode{x27D1}} \mathbf a\right)$$&lt;br /&gt;
&lt;br /&gt;
:$$[\mathbf a, \mathbf b]^{\Large\unicode{x27C7}}_- = \dfrac{1}{2}\left(\mathbf a \mathbin{\unicode{x27C7}} \mathbf b - \mathbf b \mathbin{\unicode{x27C7}} \mathbf a\right)$$&lt;br /&gt;
&lt;br /&gt;
:$$[\mathbf a, \mathbf b]^{\Large\unicode{x27C7}}_+ = \dfrac{1}{2}\left(\mathbf a \mathbin{\unicode{x27C7}} \mathbf b + \mathbf b \mathbin{\unicode{x27C7}} \mathbf a\right)$$&lt;br /&gt;
&lt;br /&gt;
Commutators provide a way to formulate [[join and meet]] operations as well as [[Euclidean distances]] between different types of geometric objects. A commutator is also used to determine a new [[line]] containing the two closest points on a pair of skew [[lines]].&lt;br /&gt;
&lt;br /&gt;
== See Also ==&lt;br /&gt;
&lt;br /&gt;
* [[Join and meet]]&lt;br /&gt;
* [[Euclidean distance]]&lt;/div&gt;</summary>
		<author><name>Eric Lengyel</name></author>
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