Impact disruption of primordial planetesimals

Autores
Parisi, Mirta Gabriela
Año de publicación
2013
Idioma
inglés
Tipo de recurso
artículo
Estado
versión publicada
Descripción
It isusually assumed that 1-10-km  sized planetesimals are formed    through coagulation processes and     continue to agglomerate via pairwise mergers. However, recent models of planetesimal formation   suggest that planetesimals of 100-1000km were produced directly from small solid particles without experiencing accretion through intermediate sizes. At present, if planetesimals were born small or big
is a matter of debate. We investigate if planetesimals in the range10-1000 km suffer growth or disruption as they collide.The collisional energy required for disruption is computed as a function of the planetesimals radius and velocity in terms of their orbital semiaxis  and eccentricity. We obtain that growth of planetesimals of  10 -100 km in the asteroid belt and the Kuiper belt requires  eccentricities much lower than what we observe today. Simulations of accretion in the terrestrial and giant planets region show that planetesimals of 10-100 km reach values of the eccentricity which lie at the disruption eccentricity limit obtained in this work. We obtain that planetesimals growth requires a very  cold disk during all the accretionary process, which seems to be difficult to achieve. We conclude that large planetesimals may be formed either invoking modern scenarios of gravitational instability or by accreting small bodies only. Planetesimals of intermediate sizes would then be the  result of disruption events. We obtain that accretion requires an impactor target mass ratio smaller than 0.1-0.01. This implies that the exponent q of the power law mass distribution of bodies must be greater than two during all the planetary formation process. However, if during oligarchic growth a bimodal mass distribution of small and large bodies exists, the mass distribution of small bodies allows q less than 2 provided the mass ratio between the largest body of such distribution and the smallest body of the distribution of large planetesimals is smaller than  0.1-0.01.
Fil: Parisi, Mirta Gabriela. Consejo Nacional de Investigaciones Científicas y Técnicas. Centro Científico Tecnológico La Plata. Instituto Argentino de Radioastronomia (i); Argentina
Materia
Solar System Formation
Planetesimals
Accretion
Nivel de accesibilidad
acceso abierto
Condiciones de uso
https://creativecommons.org/licenses/by-nc-sa/2.5/ar/
Repositorio
CONICET Digital (CONICET)
Institución
Consejo Nacional de Investigaciones Científicas y Técnicas
OAI Identificador
oai:ri.conicet.gov.ar:11336/3182

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spelling Impact disruption of primordial planetesimalsParisi, Mirta GabrielaSolar System FormationPlanetesimalsAccretionhttps://purl.org/becyt/ford/1.3https://purl.org/becyt/ford/1It isusually assumed that 1-10-km  sized planetesimals are formed    through coagulation processes and     continue to agglomerate via pairwise mergers. However, recent models of planetesimal formation   suggest that planetesimals of 100-1000km were produced directly from small solid particles without experiencing accretion through intermediate sizes. At present, if planetesimals were born small or big<br />is a matter of debate. We investigate if planetesimals in the range10-1000 km suffer growth or disruption as they collide.The collisional energy required for disruption is computed as a function of the planetesimals radius and velocity in terms of their orbital semiaxis  and eccentricity. We obtain that growth of planetesimals of  10 -100 km in the asteroid belt and the Kuiper belt requires  eccentricities much lower than what we observe today. Simulations of accretion in the terrestrial and giant planets region show that planetesimals of 10-100 km reach values of the eccentricity which lie at the disruption eccentricity limit obtained in this work. We obtain that planetesimals growth requires a very  cold disk during all the accretionary process, which seems to be difficult to achieve. We conclude that large planetesimals may be formed either invoking modern scenarios of gravitational instability or by accreting small bodies only. Planetesimals of intermediate sizes would then be the  result of disruption events. We obtain that accretion requires an impactor target mass ratio smaller than 0.1-0.01. This implies that the exponent q of the power law mass distribution of bodies must be greater than two during all the planetary formation process. However, if during oligarchic growth a bimodal mass distribution of small and large bodies exists, the mass distribution of small bodies allows q less than 2 provided the mass ratio between the largest body of such distribution and the smallest body of the distribution of large planetesimals is smaller than  0.1-0.01.Fil: Parisi, Mirta Gabriela. Consejo Nacional de Investigaciones Científicas y Técnicas. Centro Científico Tecnológico La Plata. Instituto Argentino de Radioastronomia (i); ArgentinaPergamon-elsevier Science Ltd2013-01info:eu-repo/semantics/articleinfo:eu-repo/semantics/publishedVersionhttp://purl.org/coar/resource_type/c_6501info:ar-repo/semantics/articuloapplication/pdfapplication/pdfhttp://hdl.handle.net/11336/3182Parisi, Mirta Gabriela; Impact disruption of primordial planetesimals; Pergamon-elsevier Science Ltd; Planetary And Space Science; 75; 1-2013; 96-1040032-0633enginfo:eu-repo/semantics/altIdentifier/url/http://www.sciencedirect.com/science/article/pii/S0032063312002887info:eu-repo/semantics/altIdentifier/doi/info:eu-repo/semantics/altIdentifier/url/http://dx.doi.com/10.1016/j.pss.2012.09.013info:eu-repo/semantics/openAccesshttps://creativecommons.org/licenses/by-nc-sa/2.5/ar/reponame:CONICET Digital (CONICET)instname:Consejo Nacional de Investigaciones Científicas y Técnicas2025-09-29T10:44:36Zoai:ri.conicet.gov.ar:11336/3182instacron:CONICETInstitucionalhttp://ri.conicet.gov.ar/Organismo científico-tecnológicoNo correspondehttp://ri.conicet.gov.ar/oai/requestdasensio@conicet.gov.ar; lcarlino@conicet.gov.arArgentinaNo correspondeNo correspondeNo correspondeopendoar:34982025-09-29 10:44:36.483CONICET Digital (CONICET) - Consejo Nacional de Investigaciones Científicas y Técnicasfalse
dc.title.none.fl_str_mv Impact disruption of primordial planetesimals
title Impact disruption of primordial planetesimals
spellingShingle Impact disruption of primordial planetesimals
Parisi, Mirta Gabriela
Solar System Formation
Planetesimals
Accretion
title_short Impact disruption of primordial planetesimals
title_full Impact disruption of primordial planetesimals
title_fullStr Impact disruption of primordial planetesimals
title_full_unstemmed Impact disruption of primordial planetesimals
title_sort Impact disruption of primordial planetesimals
dc.creator.none.fl_str_mv Parisi, Mirta Gabriela
author Parisi, Mirta Gabriela
author_facet Parisi, Mirta Gabriela
author_role author
dc.subject.none.fl_str_mv Solar System Formation
Planetesimals
Accretion
topic Solar System Formation
Planetesimals
Accretion
purl_subject.fl_str_mv https://purl.org/becyt/ford/1.3
https://purl.org/becyt/ford/1
dc.description.none.fl_txt_mv It isusually assumed that 1-10-km  sized planetesimals are formed    through coagulation processes and     continue to agglomerate via pairwise mergers. However, recent models of planetesimal formation   suggest that planetesimals of 100-1000km were produced directly from small solid particles without experiencing accretion through intermediate sizes. At present, if planetesimals were born small or big<br />is a matter of debate. We investigate if planetesimals in the range10-1000 km suffer growth or disruption as they collide.The collisional energy required for disruption is computed as a function of the planetesimals radius and velocity in terms of their orbital semiaxis  and eccentricity. We obtain that growth of planetesimals of  10 -100 km in the asteroid belt and the Kuiper belt requires  eccentricities much lower than what we observe today. Simulations of accretion in the terrestrial and giant planets region show that planetesimals of 10-100 km reach values of the eccentricity which lie at the disruption eccentricity limit obtained in this work. We obtain that planetesimals growth requires a very  cold disk during all the accretionary process, which seems to be difficult to achieve. We conclude that large planetesimals may be formed either invoking modern scenarios of gravitational instability or by accreting small bodies only. Planetesimals of intermediate sizes would then be the  result of disruption events. We obtain that accretion requires an impactor target mass ratio smaller than 0.1-0.01. This implies that the exponent q of the power law mass distribution of bodies must be greater than two during all the planetary formation process. However, if during oligarchic growth a bimodal mass distribution of small and large bodies exists, the mass distribution of small bodies allows q less than 2 provided the mass ratio between the largest body of such distribution and the smallest body of the distribution of large planetesimals is smaller than  0.1-0.01.
Fil: Parisi, Mirta Gabriela. Consejo Nacional de Investigaciones Científicas y Técnicas. Centro Científico Tecnológico La Plata. Instituto Argentino de Radioastronomia (i); Argentina
description It isusually assumed that 1-10-km  sized planetesimals are formed    through coagulation processes and     continue to agglomerate via pairwise mergers. However, recent models of planetesimal formation   suggest that planetesimals of 100-1000km were produced directly from small solid particles without experiencing accretion through intermediate sizes. At present, if planetesimals were born small or big<br />is a matter of debate. We investigate if planetesimals in the range10-1000 km suffer growth or disruption as they collide.The collisional energy required for disruption is computed as a function of the planetesimals radius and velocity in terms of their orbital semiaxis  and eccentricity. We obtain that growth of planetesimals of  10 -100 km in the asteroid belt and the Kuiper belt requires  eccentricities much lower than what we observe today. Simulations of accretion in the terrestrial and giant planets region show that planetesimals of 10-100 km reach values of the eccentricity which lie at the disruption eccentricity limit obtained in this work. We obtain that planetesimals growth requires a very  cold disk during all the accretionary process, which seems to be difficult to achieve. We conclude that large planetesimals may be formed either invoking modern scenarios of gravitational instability or by accreting small bodies only. Planetesimals of intermediate sizes would then be the  result of disruption events. We obtain that accretion requires an impactor target mass ratio smaller than 0.1-0.01. This implies that the exponent q of the power law mass distribution of bodies must be greater than two during all the planetary formation process. However, if during oligarchic growth a bimodal mass distribution of small and large bodies exists, the mass distribution of small bodies allows q less than 2 provided the mass ratio between the largest body of such distribution and the smallest body of the distribution of large planetesimals is smaller than  0.1-0.01.
publishDate 2013
dc.date.none.fl_str_mv 2013-01
dc.type.none.fl_str_mv info:eu-repo/semantics/article
info:eu-repo/semantics/publishedVersion
http://purl.org/coar/resource_type/c_6501
info:ar-repo/semantics/articulo
format article
status_str publishedVersion
dc.identifier.none.fl_str_mv http://hdl.handle.net/11336/3182
Parisi, Mirta Gabriela; Impact disruption of primordial planetesimals; Pergamon-elsevier Science Ltd; Planetary And Space Science; 75; 1-2013; 96-104
0032-0633
url http://hdl.handle.net/11336/3182
identifier_str_mv Parisi, Mirta Gabriela; Impact disruption of primordial planetesimals; Pergamon-elsevier Science Ltd; Planetary And Space Science; 75; 1-2013; 96-104
0032-0633
dc.language.none.fl_str_mv eng
language eng
dc.relation.none.fl_str_mv info:eu-repo/semantics/altIdentifier/url/http://www.sciencedirect.com/science/article/pii/S0032063312002887
info:eu-repo/semantics/altIdentifier/doi/
info:eu-repo/semantics/altIdentifier/url/http://dx.doi.com/10.1016/j.pss.2012.09.013
dc.rights.none.fl_str_mv info:eu-repo/semantics/openAccess
https://creativecommons.org/licenses/by-nc-sa/2.5/ar/
eu_rights_str_mv openAccess
rights_invalid_str_mv https://creativecommons.org/licenses/by-nc-sa/2.5/ar/
dc.format.none.fl_str_mv application/pdf
application/pdf
dc.publisher.none.fl_str_mv Pergamon-elsevier Science Ltd
publisher.none.fl_str_mv Pergamon-elsevier Science Ltd
dc.source.none.fl_str_mv reponame:CONICET Digital (CONICET)
instname:Consejo Nacional de Investigaciones Científicas y Técnicas
reponame_str CONICET Digital (CONICET)
collection CONICET Digital (CONICET)
instname_str Consejo Nacional de Investigaciones Científicas y Técnicas
repository.name.fl_str_mv CONICET Digital (CONICET) - Consejo Nacional de Investigaciones Científicas y Técnicas
repository.mail.fl_str_mv dasensio@conicet.gov.ar; lcarlino@conicet.gov.ar
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