Understanding Covariance in Special Relativity & Lorentz Transformations

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SUMMARY

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.

PREREQUISITES
  • Understanding of tensor analysis
  • Familiarity with Lorentz transformations
  • Basic knowledge of special relativity
  • Concept of coordinate systems in physics
NEXT STEPS
  • Study tensor properties in detail, focusing on covariant and contravariant indices
  • Explore the implications of Lorentz transformations on physical laws
  • Investigate the concept of general covariance in general relativity
  • Learn about scalar quantities and their significance in physics
USEFUL FOR

Physicists, students of theoretical physics, and anyone interested in the mathematical foundations of special relativity and tensor calculus.

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.
 
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Try wikipedia for "general covariance". It means a physical law is expressed in a form that is valid for all coordinate systems.
 
There are two possible meanings. One, as Dick has pointed out, refers to the property of a theory that its laws take the same form in any coordinate system (usually by way of being phrased in terms of tensor quantities).

Another related definition is the distinction between covariant and contravariant quantities. These are properties of tensors, or more precisely, of specific indices of a tensor. Briefly, a tensor can be expressed in a given coordinate system as an array of numbers, but in a different coordinate system the same tensor will be denoted by a different array of numbers. There are two kinds of rules for obtaining these new numbers, one for covariant quantities and another for contravariant quantities. These rules are, in a certain sense, opposite, and by putting together a contravariant and covariant quantity in a certain way, we can get a number that is the same in all coordinate systems (called a scalar) - that is, when we transform the two quantities, they transform in opposing ways so that the resulting combination stays the same.
 

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