Which rule determines the direction of gravitomagnetism?

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The direction of gravitomagnetism is determined by the right-hand rule when representing the gravitomagnetic field as a vector. Typically, a tensor formulation is employed for the combined gravitoelectric and gravitomagnetic fields, analogous to the Faraday tensor in electromagnetism. Caution is advised when transforming these representations, as the gravitomagnetic field may appear tensor-like but does not behave as one under transformation. For clarity, using the right-hand rule is recommended for vector representation.

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Do you use a left-hand or right-hand rule with gravitomagnetism?
 
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Usually people use a tensor formulation for the combined gravitoelectric and gravitomagnetic field, similar to the way that the Faraday tensor for electromagnetism combines the electric field and the magnetic field.

See http://en.wikipedia.org/w/index.php?title=Electromagnetic_tensor&oldid=150939457

for a discussion of the Faraday tensor.

However, I suppose you could represent the gravitomagnetic field as a vector, as long as you don't try and transform it as a vector (the same caution applies to the tensor form - it "looks like" a tensor, but it doesn't transform as one).

If you did chose to represent it via a vector, I'd recommend using the right hand rule.
 

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