A rod one light-year long, made as stiff as physics allows, floats at rest in front of you. You shove your end forward by one meter. When does the far end move — and if the answer were “immediately,” could you use the rod to send messages faster than light?
Solution
Some seventeen thousand years later — and no.
A perfectly rigid body is a Newtonian fiction. Your shove propagates down the rod as a compression wave at the material’s longitudinal elastic speed — for a slender rod — and relativistic causality caps every signal, elastic waves included, at . Which speed matters is set by the question: the far end first stirs when the fastest longitudinal front arrives, not at the fluid value or the slower shear speed. For diamond the compression wave runs at — the fastest of any material (the often quoted is its shear speed) — so the far end of a light-year rod answers your shove a factor later than light would: some seventeen thousand years. Stiffness is not a loophole, because the moduli are not free dials: they are coarse-grained coefficients of interatomic dynamics that is electromagnetic, hence Lorentz-invariant, and the characteristic cone of a Lorentz-invariant theory lies inside the light cone. No choice of stiffness pushes past without changing the microphysics itself.
The deeper point is that relativity does not merely forbid building a rigid rod; it forbids defining one that can be commanded from one end. The strongest rigidity the theory admits — Born rigidity, constant proper distance between neighboring pieces as measured in their momentarily comoving frames — is so restrictive that prescribing one point’s worldline already fixes the entire body, and any rotating rigid motion is frozen into a Killing flow outright (this is the Herglotz–Noether theorem). Even the surviving freedom is no loophole: the far end’s motion is determined by the near end’s whole worldline, future included. It is a global consistency condition laid down in advance, not a response propagated from your hand — change your mind mid-push and the motion was never Born-rigid to begin with.
Deeper in the notebook: 01. Timelike, Null and Spacelike Separation; the Causal Order · 03. Tachyons and the Limits of Causality (signpost) · 03. Bell’s Spaceship Paradox and Born Rigidity