{"title":"从滑行到能量守恒:强爆炸相互作用阶段的新自相似解","authors":"Eric R. Coughlin","doi":"arxiv-2409.10600","DOIUrl":null,"url":null,"abstract":"Astrophysical explosions that contain dense and ram-pressure-dominated ejecta\nevolve through an interaction phase, during which a forward shock (FS), contact\ndiscontinuity (CD), and reverse shock (RS) form and expand with time. We\ndescribe new self-similar solutions that apply to this phase and are most\naccurate in the limit that the ejecta density is large compared to the ambient\ndensity. These solutions predict that the FS, CD, and RS expand at different\nrates in time and not as single temporal power-laws, are valid for explosions\ndriven by steady winds and homologously expanding ejecta, and exist when the\nambient density profile is a power-law with power-law index shallower than\n$\\sim 3$ (specifically when the FS does not accelerate). We find excellent\nagreement between the predictions of these solutions and hydrodynamical\nsimulations, both for the temporal behavior of the discontinuities and for the\nvariation of the fluid quantities. The self-similar solutions are applicable to\na wide range of astrophysical phenomena and -- although the details are\ndescribed in future work -- can be generalized to incorporate relativistic\nspeeds with arbitrary Lorentz factors. We suggest that these solutions\naccurately interpolate between the initial ``coasting'' phase of the explosion\nand the later, energy-conserving phase (or, if the ejecta is homologous and the\ndensity profile is sufficiently steep, the self-similar phase described in\nChevalier 1982),","PeriodicalId":501343,"journal":{"name":"arXiv - PHYS - High Energy Astrophysical Phenomena","volume":"29 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-09-16","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"From coasting to energy-conserving: new self-similar solutions to the interaction phase of strong explosions\",\"authors\":\"Eric R. Coughlin\",\"doi\":\"arxiv-2409.10600\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Astrophysical explosions that contain dense and ram-pressure-dominated ejecta\\nevolve through an interaction phase, during which a forward shock (FS), contact\\ndiscontinuity (CD), and reverse shock (RS) form and expand with time. We\\ndescribe new self-similar solutions that apply to this phase and are most\\naccurate in the limit that the ejecta density is large compared to the ambient\\ndensity. These solutions predict that the FS, CD, and RS expand at different\\nrates in time and not as single temporal power-laws, are valid for explosions\\ndriven by steady winds and homologously expanding ejecta, and exist when the\\nambient density profile is a power-law with power-law index shallower than\\n$\\\\sim 3$ (specifically when the FS does not accelerate). We find excellent\\nagreement between the predictions of these solutions and hydrodynamical\\nsimulations, both for the temporal behavior of the discontinuities and for the\\nvariation of the fluid quantities. The self-similar solutions are applicable to\\na wide range of astrophysical phenomena and -- although the details are\\ndescribed in future work -- can be generalized to incorporate relativistic\\nspeeds with arbitrary Lorentz factors. We suggest that these solutions\\naccurately interpolate between the initial ``coasting'' phase of the explosion\\nand the later, energy-conserving phase (or, if the ejecta is homologous and the\\ndensity profile is sufficiently steep, the self-similar phase described in\\nChevalier 1982),\",\"PeriodicalId\":501343,\"journal\":{\"name\":\"arXiv - PHYS - High Energy Astrophysical Phenomena\",\"volume\":\"29 1\",\"pages\":\"\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2024-09-16\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"arXiv - PHYS - High Energy Astrophysical Phenomena\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/arxiv-2409.10600\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"arXiv - PHYS - High Energy Astrophysical Phenomena","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/arxiv-2409.10600","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
From coasting to energy-conserving: new self-similar solutions to the interaction phase of strong explosions
Astrophysical explosions that contain dense and ram-pressure-dominated ejecta
evolve through an interaction phase, during which a forward shock (FS), contact
discontinuity (CD), and reverse shock (RS) form and expand with time. We
describe new self-similar solutions that apply to this phase and are most
accurate in the limit that the ejecta density is large compared to the ambient
density. These solutions predict that the FS, CD, and RS expand at different
rates in time and not as single temporal power-laws, are valid for explosions
driven by steady winds and homologously expanding ejecta, and exist when the
ambient density profile is a power-law with power-law index shallower than
$\sim 3$ (specifically when the FS does not accelerate). We find excellent
agreement between the predictions of these solutions and hydrodynamical
simulations, both for the temporal behavior of the discontinuities and for the
variation of the fluid quantities. The self-similar solutions are applicable to
a wide range of astrophysical phenomena and -- although the details are
described in future work -- can be generalized to incorporate relativistic
speeds with arbitrary Lorentz factors. We suggest that these solutions
accurately interpolate between the initial ``coasting'' phase of the explosion
and the later, energy-conserving phase (or, if the ejecta is homologous and the
density profile is sufficiently steep, the self-similar phase described in
Chevalier 1982),