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Costa, João L. & Natário, J (2019). Elastic shocks in relativistic rigid rods and balls. Proceedings of the Royal Society A: Mathematical, Physical and Engineering Sciences. 475 (2225), 1-17

J. L. Costa and J. Natário,  "Elastic shocks in relativistic rigid rods and balls", in Proc. of the Royal Society A: Mathematical, Physical and Engineering Sciences, vol. 475, no. 2225, pp. 1-17, 2019

@article{costa2019_1714713029479,
	author = "Costa, João L. and Natário, J",
	title = "Elastic shocks in relativistic rigid rods and balls",
	journal = "Proceedings of the Royal Society A: Mathematical, Physical and Engineering Sciences",
	year = "2019",
	volume = "475",
	number = "2225",
	doi = "10.1098/rspa.2018.0858",
	pages = "1-17",
	url = "https://royalsocietypublishing.org/doi/10.1098/rspa.2018.0858"
}

TY  - JOUR
TI  - Elastic shocks in relativistic rigid rods and balls
T2  - Proceedings of the Royal Society A: Mathematical, Physical and Engineering Sciences
VL  - 475
IS  - 2225
AU  - Costa, João L.
AU  - Natário, J
PY  - 2019
SP  - 1-17
SN  - 1364-5021
DO  - 10.1098/rspa.2018.0858
UR  - https://royalsocietypublishing.org/doi/10.1098/rspa.2018.0858
AB  - We study the free boundary problem for the ‘hard phase’ material introduced by Christodoulou in (Christodoulou 1995 Arch. Ration. Mech. Anal.130, 343–400), both for rods in (1 + 1)-dimensional Minkowski space–time and for spherically symmetric balls in (3 + 1)-dimensional Minkowski space–time. Unlike Christodoulou, we do not consider a ‘soft phase’, and so we regard this material as an elastic medium, capable of both compression and stretching. We prove that shocks must be null hypersurfaces, and derive the conditions to be satisfied at a free boundary. We solve the equations of motion of the rods explicitly, and we prove existence of solutions to the equations of motion of the spherically symmetric balls for an arbitrarily long (but finite) time, given initial conditions sufficiently close to those for the relaxed ball at rest. In both cases we find that the solutions contain shocks if and only if the pressure or its time derivative do not vanish at the free boundary initially. These shocks interact with the free boundary, causing it to lose regularity.
ER  -