ehrenfest
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Can someone explain to me what it means to be "covariant" in the context of special relativity and Lorentz transformations? I already checked wikipedia.
Covariance in the context of special relativity and Lorentz transformations refers to the property that physical laws maintain the same form across all coordinate systems, typically expressed using tensor quantities. The discussion highlights two definitions: the first emphasizes the invariance of laws in different coordinate systems, while the second distinguishes between covariant and contravariant quantities, which are specific properties of tensors. Covariant quantities transform in one manner, while contravariant quantities transform oppositely, allowing for the combination of both to yield a scalar that remains invariant across transformations.
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