Simple physical models of a measuring rod and of a clock are used to demonstrate the contraction of objects and clock retardation in special relativity. It is argued that models can help student understanding of special relativity and distinguishing between dynamical and purely perspectival effects.

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In deriving Eq. (7), it has been assumed that the speed of S with respect to S¯ is v. This result follows from the method of clock synchronization we have assumed. It is less desirable to rely on the principle of reciprocity, which requires attributing some properties to space and time that are best to avoid in a constructive approach to special relativity.
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The acceleration could be achieved by immersing the apparatus in a uniform gravitational field for the required period of time (a gravitational field in which tidal effects are negligible over the dimensions of the apparatus).
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In the argument here it is tacitly assumed that if all the physical fields are Lorentz invariant, then all the laws of physics involving them must be Lorentz invariant.
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