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Proof of the Cartan Bianchi Identity

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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

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