A parameter for a family of steady vortex ring cores
Streamlined orthogonal coordinates are derived for the core of Hill’s spherical vortex. Each core boundary of Norbury’s family of vortex rings is a scaled streamline from Hill’s spherical vortex. A formula is given that relates the dimensionless mean core radius of each member of this family to its...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Morton, Thad S. [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2016 |
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| Schlagwörter: |
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| Umfang: |
5 |
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| Übergeordnetes Werk: |
Enthalten in: Global organic carbon emissions from primary sources from 1960 to 2009 - Huang, Ye ELSEVIER, 2015transfer abstract, Paris |
|---|---|
| Übergeordnetes Werk: |
volume:56 ; year:2016 ; pages:66-70 ; extent:5 |
| Links: |
|---|
| DOI / URN: |
10.1016/j.euromechflu.2015.11.001 |
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ELV029932157 |
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| 520 | |a Streamlined orthogonal coordinates are derived for the core of Hill’s spherical vortex. Each core boundary of Norbury’s family of vortex rings is a scaled streamline from Hill’s spherical vortex. A formula is given that relates the dimensionless mean core radius of each member of this family to its boundary. A new dimensionless mean core radius for vortex rings is presented that varies between 0 and 1 rather than 0 and the square root of 2, and requires that fewer geometrical parameters be specified in order to uniquely define the core area for each member of the family of vortex rings. | ||
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10.1016/j.euromechflu.2015.11.001 doi GBVA2016017000020.pica (DE-627)ELV029932157 (ELSEVIER)S0997-7546(15)00117-X DE-627 ger DE-627 rakwb eng 530 530 DE-600 550 VZ 690 VZ 610 VZ 44.65 bkl Morton, Thad S. verfasserin aut A parameter for a family of steady vortex ring cores 2016 5 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier Streamlined orthogonal coordinates are derived for the core of Hill’s spherical vortex. Each core boundary of Norbury’s family of vortex rings is a scaled streamline from Hill’s spherical vortex. A formula is given that relates the dimensionless mean core radius of each member of this family to its boundary. A new dimensionless mean core radius for vortex rings is presented that varies between 0 and 1 rather than 0 and the square root of 2, and requires that fewer geometrical parameters be specified in order to uniquely define the core area for each member of the family of vortex rings. Axisymmetric vortex Elsevier Hill’s spherical vortex Elsevier Streamline coordinate systems Elsevier Toroidal vortex ring Elsevier Enthalten in Gauthier-Villars Huang, Ye ELSEVIER Global organic carbon emissions from primary sources from 1960 to 2009 2015transfer abstract Paris (DE-627)ELV01880182X volume:56 year:2016 pages:66-70 extent:5 https://doi.org/10.1016/j.euromechflu.2015.11.001 Volltext GBV_USEFLAG_U GBV_ELV SYSFLAG_U SSG-OLC-PHA GBV_ILN_40 GBV_ILN_70 44.65 Chirurgie VZ AR 56 2016 66-70 5 045F 530 |
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10.1016/j.euromechflu.2015.11.001 doi GBVA2016017000020.pica (DE-627)ELV029932157 (ELSEVIER)S0997-7546(15)00117-X DE-627 ger DE-627 rakwb eng 530 530 DE-600 550 VZ 690 VZ 610 VZ 44.65 bkl Morton, Thad S. verfasserin aut A parameter for a family of steady vortex ring cores 2016 5 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier Streamlined orthogonal coordinates are derived for the core of Hill’s spherical vortex. Each core boundary of Norbury’s family of vortex rings is a scaled streamline from Hill’s spherical vortex. A formula is given that relates the dimensionless mean core radius of each member of this family to its boundary. A new dimensionless mean core radius for vortex rings is presented that varies between 0 and 1 rather than 0 and the square root of 2, and requires that fewer geometrical parameters be specified in order to uniquely define the core area for each member of the family of vortex rings. Axisymmetric vortex Elsevier Hill’s spherical vortex Elsevier Streamline coordinate systems Elsevier Toroidal vortex ring Elsevier Enthalten in Gauthier-Villars Huang, Ye ELSEVIER Global organic carbon emissions from primary sources from 1960 to 2009 2015transfer abstract Paris (DE-627)ELV01880182X volume:56 year:2016 pages:66-70 extent:5 https://doi.org/10.1016/j.euromechflu.2015.11.001 Volltext GBV_USEFLAG_U GBV_ELV SYSFLAG_U SSG-OLC-PHA GBV_ILN_40 GBV_ILN_70 44.65 Chirurgie VZ AR 56 2016 66-70 5 045F 530 |
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Streamlined orthogonal coordinates are derived for the core of Hill’s spherical vortex. Each core boundary of Norbury’s family of vortex rings is a scaled streamline from Hill’s spherical vortex. A formula is given that relates the dimensionless mean core radius of each member of this family to its boundary. A new dimensionless mean core radius for vortex rings is presented that varies between 0 and 1 rather than 0 and the square root of 2, and requires that fewer geometrical parameters be specified in order to uniquely define the core area for each member of the family of vortex rings. |
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Streamlined orthogonal coordinates are derived for the core of Hill’s spherical vortex. Each core boundary of Norbury’s family of vortex rings is a scaled streamline from Hill’s spherical vortex. A formula is given that relates the dimensionless mean core radius of each member of this family to its boundary. A new dimensionless mean core radius for vortex rings is presented that varies between 0 and 1 rather than 0 and the square root of 2, and requires that fewer geometrical parameters be specified in order to uniquely define the core area for each member of the family of vortex rings. |
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Streamlined orthogonal coordinates are derived for the core of Hill’s spherical vortex. Each core boundary of Norbury’s family of vortex rings is a scaled streamline from Hill’s spherical vortex. A formula is given that relates the dimensionless mean core radius of each member of this family to its boundary. A new dimensionless mean core radius for vortex rings is presented that varies between 0 and 1 rather than 0 and the square root of 2, and requires that fewer geometrical parameters be specified in order to uniquely define the core area for each member of the family of vortex rings. |
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