2021
DOI: 10.48550/arxiv.2104.11131
|View full text |Cite
Preprint
|
Sign up to set email alerts
|

Self-gravitating static balls of power-law elastic matter

Artur Alho,
Simone Calogero,
Astrid Liljenberg

Abstract: We study a class of power-law stored energy functions for spherically symmetric elastic bodies that includes well-known material models, such as the Saint Venant-Kirchhoff, Hadamard, Signorini and John models. We identify a finite subclass of these stored energy functions, which we call Lamé type, that depend on no more material parameters than the bulk modulus κ > 0 and the Poisson ratio −1 < ν ≤ 1/2. A general theorem proving the existence of static self-gravitating elastic balls for some power-law materials… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1

Citation Types

0
2
0

Year Published

2021
2021
2022
2022

Publication Types

Select...
1
1

Relationship

2
0

Authors

Journals

citations
Cited by 2 publications
(2 citation statements)
references
References 11 publications
(23 reference statements)
0
2
0
Order By: Relevance
“…Here s can be interpreted as the shear index; when s ¼ n and ε ¼ 0 we recover the usual relativistic polytropes (see also [34,35] for similar stored energy functions in the Newtonian setting). The Lamé parameters are the same as in the quadratic model (12), and in fact the two models coincide when s ¼ n ¼ 1.…”
Section: Materials Modelsmentioning
confidence: 85%
“…Here s can be interpreted as the shear index; when s ¼ n and ε ¼ 0 we recover the usual relativistic polytropes (see also [34,35] for similar stored energy functions in the Newtonian setting). The Lamé parameters are the same as in the quadratic model (12), and in fact the two models coincide when s ¼ n ¼ 1.…”
Section: Materials Modelsmentioning
confidence: 85%
“…Here s can be interpreted as the shear index; when s = n and ε = 0 we recover the usual relativistic polytropes. This function w(δ, η) is similar to the power-law stored energy function (2.18) in [33], which belongs to a more general class of polytropic elastic materials introduced (11) with n = 1/2 and K = 6 × 10 4 M 4 (left) and for the two-parameter elastic model (12) with n = 1 and K = 100M 2 (right). Solid (dashed) curves correspond to configurations with subluminal (superluminal) wave propagation.…”
Section: Introductionmentioning
confidence: 93%