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DEFINITIVE PROOF 4 : THE CARTAN BIANCHI IDENTITY<br />
The <strong>Cartan</strong> <strong>Bianchi</strong> identity was first introduced by <strong>Cartan</strong> in about 1925 and has<br />
been a standard feature <strong>of</strong> <strong>Cartan</strong> geometry ever since. It is a rigorously correct identity<br />
based on <strong>the</strong> definitions <strong>of</strong> <strong>the</strong> curvature and torsion tensors introduced in Definitive <strong>Pro<strong>of</strong></strong><br />
2. As always in <strong>Cartan</strong> geometry it relies on <strong>the</strong> tetrad postulate without loss <strong>of</strong> generality.<br />
It links toge<strong>the</strong>r torsion and curvature and torsion, and is <strong>the</strong> basis <strong>of</strong> <strong>the</strong> homogeneous<br />
field equations <strong>of</strong> both dynamics and electrodynamics in ECE <strong>the</strong>ory.<br />
<strong>Pro<strong>of</strong></strong>.<br />
In standard differential form notation (see Carroll, chapter 3) <strong>the</strong> identity is:<br />
d˄ + ˄ : = ˄ (1)<br />
which translates into tensor notation as follows:<br />
∂ρ + ∂ρ + ∂ρ + ρ + ρ + ρ : =<br />
where:<br />
and so on. Using Leibniz Theorem:<br />
<br />
( ρ + ρ + ρ ) (2)<br />
<br />
ρ = ( Гρ - Гρ ) (3)<br />
∂ρ = (∂Гρ - ∂Гρ ) + ( Гρ - Гρ ) ∂ (4)<br />
and so on. Therefore, Eq. (2) becomes:<br />
(∂Гρ - ∂Гρ ) + ( Гρ - Гρ ) (∂ + <br />
) + : =<br />
<br />
( ρ + ρ + ρ ) (5)<br />
Now relabel repeated summation indices (dummy indices) as follows:<br />
to obtain:<br />
λ → σ (6)<br />
1
(∂Гρ - ∂Гρ ) + ( Гρ - Гρ ) (∂ + <br />
) + : =<br />
Use <strong>the</strong> tetrad postulate to obtain:<br />
∂Гρ - ∂Гρ + Г ( Гρ - Гρ ) +<br />
∂ρГ - ∂ρГ + Гρ ( Г - Г ) +<br />
<br />
( ρ + ρ + ρ ) (7)<br />
∂Гρ - ∂Гρ + Г ( Гρ - Гρ ) : = ρ + ρ + ρ (8)<br />
and re-arrange:<br />
ρ + ρ + ρ : =<br />
∂Гρ - ∂Гρ + Г Гρ - Г Гρ +<br />
∂Гρ - ∂ρГ + Г Гρ - Гρ Г +<br />
∂ρГ - ∂Гρ + Гρ Г - Г Гρ<br />
(9)<br />
This is an exact identity because <strong>the</strong> curvature tensors on <strong>the</strong> left hand side are<br />
defined by:<br />
<br />
ρ = ∂Гρ - ∂ρГ + Г Гρ - Гρ Г<br />
<br />
ρ = ∂ρГ - ∂Гρ + Гρ Г - Г Гρ<br />
ρ = ∂Гρ - ∂Гρ + Г Гρ - Г Гρ<br />
(10)<br />
Quod erat demonstrandum.<br />
2