| 1. | The force's vector components are also three in number.
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| 2. | Two scalar components and one vector component can further be eliminated by gauge transformations.
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| 3. | All the matrices are represented with the vector components in a certain frame k.
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| 4. | As per Jerry Fitzpatrick, we can assume the three vector components to be orthogonal.
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| 5. | They will also auto-range themselves based on the maximum and minimum of each vector component.
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| 6. | This means that they have both covariant and contravariant components, or both vector and dual vector components.
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| 7. | In particular, the conserved LRL vector component " A s " corresponds to the variation in the coordinates
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| 8. | The-vector component can be identified with the inner product and the-vector component with the outer product.
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| 9. | The-vector component can be identified with the inner product and the-vector component with the outer product.
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| 10. | However, the vector components are generally ignored, as there are few known physical processes in which they can be generated.
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