Supersonic Gravitational Collapse for Nonisentropic Gaseous Stars

We show the existence of a new class of initially smooth spherically symmetric self-similar solutions to the non-isentropic Euler--Poisson system. These solutions exhibit supersonic gravitational implosion in the sense that the density blows-up in finite time while the fluid velocity remains supersonic. In particular, they occupy a portion of the phase space that is far from the recently constructed isentropic self-similar implosion. At the heart of our proof is the presence of a two-parameter scaling invariance and the reduction of the problem to a non-autonomous system of ordinary differential equations. We use the requirement of smoothness of the flow as a selection principle that constrains the choice of scaling indices. An important consequence of our analysis is that for all the solutions we construct, the polytropic index $\ga$ is strictly bigger than $\frac{4}{3}$, which is in sharp contrast to the known results in the isentropic case.

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Publication Details

Journal
SIAM Journal on Mathematical Analysis
Published
2025-06-24
DOI
https://doi.org/10.1137/24m1701617
Primary Topic
Astrophysics and Star Formation Studies
Type
article
Field-Weighted Citation Impact
0.00

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article

Supersonic Gravitational Collapse for Nonisentropic Gaseous Stars

Matthew Schrecker, Mahir Hadžić, Christopher Alexander
SIAM Journal on Mathematical Analysis
Astrophysics and Star Formation Studies
article

Supersonic Gravitational Collapse for Nonisentropic Gaseous Stars

Matthew Schrecker, Mahir Hadžić, Christopher Alexander
article en

Abstract

We show the existence of a new class of initially smooth spherically symmetric self-similar solutions to the non-isentropic Euler--Poisson system. These solutions exhibit supersonic gravitational implosion in the sense that the density blows-up in finite time while the fluid velocity remains supersonic. In particular, they occupy a portion of the phase space that is far from the recently constructed isentropic self-similar implosion. At the heart of our proof is the presence of a two-parameter scaling invariance and the reduction of the problem to a non-autonomous system of ordinary differential equations. We use the requirement of smoothness of the flow as a selection principle that constrains the choice of scaling indices. An important consequence of our analysis is that for all the solutions we construct, the polytropic index $\ga$ is strictly bigger than $\frac{4}{3}$, which is in sharp contrast to the known results in the isentropic case.

SIAM Journal on Mathematical AnalysisVol. 57(3)
University College London (GB), University of Bath (GB)
Engineering and Physical Sciences Research Council
Climate action
Openalex Percentile: Top 91%
Astrophysics and Star Formation Studies
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