10Electromagnetic Fields

10.1 Theory

In Clifford algebra, electromagnetic fields are represented1 by identifying the temporal unit vector ModifyingAbove bold t With bold Ì‚ and the spatial unit vectors ModifyingAbove bold x With bold Ì‚ comma ModifyingAbove bold y With bold Ì‚ comma ModifyingAbove bold z With bold Ì‚ with particular Clifford units:

(10.1)StartLayout Enlarged left-brace 1st Row 1st Column ModifyingAbove bold t With bold Ì‚ 2nd Column left-right-arrow 3rd Column i e 0 2nd Row 1st Column ModifyingAbove bold x With bold Ì‚ 2nd Column left-right-arrow 3rd Column e 1 3rd Row 1st Column ModifyingAbove bold y With bold Ì‚ 2nd Column left-right-arrow 3rd Column e 2 4th Row 1st Column ModifyingAbove bold z With bold Ì‚ 2nd Column left-right-arrow 3rd Column e 3 EndLayout

in a context, where the signature lamda is all negative 1.

Four dimensions are required, with the extra dimension used for time or frequency. The Clifford unit for time is imaginary rather than real so that the Clifford geometry with uniform signatures behaves like the Minkowskian geometry, which has mixed signatures.2

Electromagnetic fields in four dimensions form a particular subset of four‐dimensional Clifford numbers. Although four‐dimensional Clifford numbers have 5 grades and 16 components, electromagnetic fields retain only one of the grades (grade 2) and six of the components. Three of these components are used to accommodate the magnetic field, and the other three are used for the electric field.

10.1.1 Time and Frequency

Electromagnetic fields are in general functions of both three‐dimensional ...

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