Turbulent transport and entrainment in jets and plumes: A DNS study
We present a direct numerical simulation (DNS) data set for a statistically axisymmetric turbulent jet, plume, and forced plume in a domain of size 40r 0 × 40r 0 × 60r 0 , where r 0 is the source diameter. The data set supports the validity of the Priestley-Ball entrainment model in unstratified env...
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description | We present a direct numerical simulation (DNS) data set for a statistically axisymmetric turbulent jet, plume, and forced plume in a domain of size 40r 0 × 40r 0 × 60r 0 , where r 0 is the source diameter. The data set supports the validity of the Priestley-Ball entrainment model in unstratified environments (excluding the region near the source) [Priestley and Ball, Q. J. R. Meteor. Soc. 81, 144 (1955)], which is corroborated further by the Wang-Law and Ezzamel et al. experimental data sets [Wang and Law, J. Fluid Mech. 459, 397 (2002); Ezzamel et al., ibid. 765, 576 (2015)], the latter being corrected for a small but influential coflow that affected the statistics. We show that the second-order turbulence statistics in the core region of the jet and the plume are practically indistinguishable from each other, although there are significant differences near the plume edge. The DNS data indicate that the turbulent Prandtl number is about 0.7 for both jets and plumes. For plumes, this value is a result of the difference in the ratio of the radial turbulent transport of radial momentum and buoyancy. For jets, however, the value originates from a different spread of the buoyancy and velocity profiles, in spite of the fact that the ratio of radial turbulent transport terms is approximately unity. The DNS data do not show any evidence of similarity drift associated with gradual variations in the ratio of buoyancy profile to velocity profile widths. |
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The data set supports the validity of the Priestley-Ball entrainment model in unstratified environments (excluding the region near the source) [Priestley and Ball, Q. J. R. Meteor. Soc. 81, 144 (1955)], which is corroborated further by the Wang-Law and Ezzamel et al. experimental data sets [Wang and Law, J. Fluid Mech. 459, 397 (2002); Ezzamel et al., ibid. 765, 576 (2015)], the latter being corrected for a small but influential coflow that affected the statistics. We show that the second-order turbulence statistics in the core region of the jet and the plume are practically indistinguishable from each other, although there are significant differences near the plume edge. The DNS data indicate that the turbulent Prandtl number is about 0.7 for both jets and plumes. For plumes, this value is a result of the difference in the ratio of the radial turbulent transport of radial momentum and buoyancy. For jets, however, the value originates from a different spread of the buoyancy and velocity profiles, in spite of the fact that the ratio of radial turbulent transport terms is approximately unity. 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The data set supports the validity of the Priestley-Ball entrainment model in unstratified environments (excluding the region near the source) [Priestley and Ball, Q. J. R. Meteor. Soc. 81, 144 (1955)], which is corroborated further by the Wang-Law and Ezzamel et al. experimental data sets [Wang and Law, J. Fluid Mech. 459, 397 (2002); Ezzamel et al., ibid. 765, 576 (2015)], the latter being corrected for a small but influential coflow that affected the statistics. We show that the second-order turbulence statistics in the core region of the jet and the plume are practically indistinguishable from each other, although there are significant differences near the plume edge. The DNS data indicate that the turbulent Prandtl number is about 0.7 for both jets and plumes. For plumes, this value is a result of the difference in the ratio of the radial turbulent transport of radial momentum and buoyancy. For jets, however, the value originates from a different spread of the buoyancy and velocity profiles, in spite of the fact that the ratio of radial turbulent transport terms is approximately unity. The DNS data do not show any evidence of similarity drift associated with gradual variations in the ratio of buoyancy profile to velocity profile widths.</description><subject>Fluid mechanics</subject><subject>Mechanics</subject><subject>Physics</subject><issn>2469-990X</issn><issn>2469-990X</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2016</creationdate><recordtype>article</recordtype><recordid>eNpVkFFLwzAQx4MoOOa-guTVh867Jksb38Z0TigqOsG3kDYJ62i7kbSDfns7J6JPd_e7_93Dj5BrhCkisNvXTR_e7GFZdaUJU5xCwhngGRnFXMhISvg8_9NfkkkIWwBAwZJEpiOyWHc-7yrbtLT1ugn7nW-pbgwdiNdlUx83ZUO3tg3ffF91tQ13dE7vn99paDvTX5ELp6tgJz91TD6WD-vFKspeHp8W8ywqmIQ2SmaCs9ik0hkOaG0udeqMZaLQhUGeaxvnblYIjVYnQuYpT1nspDTDFINL2JjcnP5udKX2vqy179VOl2o1z9SRAc5QgOQHHLLilC38LgRv3e8BgjqaU__MKVQnc-wLeJdlnw</recordid><startdate>20161101</startdate><enddate>20161101</enddate><creator>van Reeuwijk, Maarten</creator><creator>Salizzoni, Pietro</creator><creator>Hunt, Gary R.</creator><creator>Craske, John</creator><general>American Physical Society</general><scope>AAYXX</scope><scope>CITATION</scope><scope>1XC</scope><scope>VOOES</scope></search><sort><creationdate>20161101</creationdate><title>Turbulent transport and entrainment in jets and plumes: A DNS study</title><author>van Reeuwijk, Maarten ; Salizzoni, Pietro ; Hunt, Gary R. ; Craske, John</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c390t-756432d89fd401eeb9a8fde36cacd14bae2bf5c6a1ea769b84832f99da7620f73</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2016</creationdate><topic>Fluid mechanics</topic><topic>Mechanics</topic><topic>Physics</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>van Reeuwijk, Maarten</creatorcontrib><creatorcontrib>Salizzoni, Pietro</creatorcontrib><creatorcontrib>Hunt, Gary R.</creatorcontrib><creatorcontrib>Craske, John</creatorcontrib><collection>CrossRef</collection><collection>Hyper Article en Ligne (HAL)</collection><collection>Hyper Article en Ligne (HAL) (Open Access)</collection><jtitle>Physical review fluids</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>van Reeuwijk, Maarten</au><au>Salizzoni, Pietro</au><au>Hunt, Gary R.</au><au>Craske, John</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Turbulent transport and entrainment in jets and plumes: A DNS study</atitle><jtitle>Physical review fluids</jtitle><date>2016-11-01</date><risdate>2016</risdate><volume>1</volume><issue>7</issue><artnum>074301</artnum><issn>2469-990X</issn><eissn>2469-990X</eissn><abstract>We present a direct numerical simulation (DNS) data set for a statistically axisymmetric turbulent jet, plume, and forced plume in a domain of size 40r 0 × 40r 0 × 60r 0 , where r 0 is the source diameter. The data set supports the validity of the Priestley-Ball entrainment model in unstratified environments (excluding the region near the source) [Priestley and Ball, Q. J. R. Meteor. Soc. 81, 144 (1955)], which is corroborated further by the Wang-Law and Ezzamel et al. experimental data sets [Wang and Law, J. Fluid Mech. 459, 397 (2002); Ezzamel et al., ibid. 765, 576 (2015)], the latter being corrected for a small but influential coflow that affected the statistics. We show that the second-order turbulence statistics in the core region of the jet and the plume are practically indistinguishable from each other, although there are significant differences near the plume edge. The DNS data indicate that the turbulent Prandtl number is about 0.7 for both jets and plumes. For plumes, this value is a result of the difference in the ratio of the radial turbulent transport of radial momentum and buoyancy. For jets, however, the value originates from a different spread of the buoyancy and velocity profiles, in spite of the fact that the ratio of radial turbulent transport terms is approximately unity. The DNS data do not show any evidence of similarity drift associated with gradual variations in the ratio of buoyancy profile to velocity profile widths.</abstract><pub>American Physical Society</pub><doi>10.1103/PhysRevFluids.1.074301</doi><oa>free_for_read</oa></addata></record> |
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title | Turbulent transport and entrainment in jets and plumes: A DNS study |
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