The Special Del and the Generalized Del: Difference between revisions
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| published = 2009 | | published = 2009 | ||
| journal = [[Galilean Electrodynamics]] | | journal = [[Galilean Electrodynamics]] | ||
| volume = | | volume = 20 | ||
| number = | | number = 6 | ||
| pages = 106-109 | | pages = 106-109 | ||
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Latest revision as of 09:40, 21 July 2026
| Scientific Paper | |
|---|---|
| Title | The Special Del and the Generalized Del |
| Author(s) | [[]] |
| Keywords | del, nabla, Hamiltonian, vector analysis, tensor analysis |
| Published | 2009 |
| Journal | Galilean Electrodynamics |
| Volume | 20 |
| Number | 6 |
| Pages | 106-109 |
Abstract
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.