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Spin Connection Resonance in the Bedini Machine - Alpha Institute ...

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A<br />

Appendix 1: Reduction of Form Notation to<br />

Vector Notation<br />

In differential form notation <strong>the</strong> electromagnetic field <strong>in</strong> ECE <strong>the</strong>ory is:<br />

which <strong>in</strong> tensor notation is 1–10:<br />

The electromagnetic potential is:<br />

F a = d ∧ A a + ω a b ∧ A b<br />

(A.1)<br />

F a µν = ∂µA a ν − ∂νA a µ + ω a µbA b ν − ω a νbA b µ. (A.2)<br />

A a µ = A (0) q a µ<br />

where q a µ is a rank two mixed <strong>in</strong>dex tensor def<strong>in</strong>ed by:<br />

(A.3)<br />

V a = q a µV µ . (A.4)<br />

Here V a and V µ are four vectors <strong>in</strong> different frames of reference labeled a and<br />

µ <strong>in</strong> four dimensional space-time. Consider a particular example of Eq. (A.2):<br />

F 1 23 = ∂2A 1 3 − ∂3A 1 2 + ω 1 2bA b 3 − ω 1 3bA b 2. (A.5)<br />

Ei<strong>the</strong>r side of <strong>the</strong> equation <strong>the</strong>re are rank three tensors whose components<br />

must correspond to each o<strong>the</strong>r on both sides. Thus:<br />

F 1 23 =(∂2A3 − ∂3A2) 1 + ω2bA b 3 − ω3bA b 2<br />

1 . (A.6)<br />

Inside <strong>the</strong> brackets on <strong>the</strong> right hand side are anti-symmetric tensor components<br />

which correspond to <strong>the</strong> components of an axial vector (magnetic field)

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