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	<title>The Special Del and the Generalized Del - Revision history</title>
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&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;{{Infobox paper&lt;br /&gt;
| title = The Special Del and the Generalized Del&lt;br /&gt;
| author = [[]]&lt;br /&gt;
| keywords = [[del]], [[nabla]], [[Hamiltonian]], [[vector analysis]], [[tensor analysis]]&lt;br /&gt;
| published = 2009&lt;br /&gt;
| journal = [[Galilean Electrodynamics]]&lt;br /&gt;
| volume = [[20]]&lt;br /&gt;
| number = [[6]]&lt;br /&gt;
| pages = 106-109&lt;br /&gt;
}}&lt;br /&gt;
&lt;br /&gt;
==Abstract==&lt;br /&gt;
&lt;br /&gt;
The Special Del is a vector partial differential operator in Cartesian coordinates, put forward by William Rowan Hamilton. The Generalized Del is a vector displacement partial differential operator in general or-thogonal curvilinear coordinates. When the result of the Special Del operating on a tensor is still a tensor, it can be replaced with Generalized Del; if not, it cannot be replaced with a Generalized Del. This paper is very important for unifying symbols concerning field theory and teaching and for learning electromagnetic theory.&lt;br /&gt;
&lt;br /&gt;
[[Category:Scientific Paper|special del generalized del]]&lt;/div&gt;</summary>
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