Characterising line fountains
We present analytical solutions for the initial rise height zm of two-dimensional turbulent fountains issuing from a horizontal linear source of width 2b0 into a quiescent environment of uniform density. Using the initial rise height prediction as a measure we classify line fountains into three type...
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Published in | Journal of fluid mechanics Vol. 623; pp. 317 - 327 |
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Main Authors | , |
Format | Journal Article |
Language | English |
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Cambridge, UK
Cambridge University Press
25.03.2009
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Abstract | We present analytical solutions for the initial rise height zm of two-dimensional turbulent fountains issuing from a horizontal linear source of width 2b0 into a quiescent environment of uniform density. Using the initial rise height prediction as a measure we classify line fountains into three types depending on their source conditions. For source Froude numbers Fr0 ≫ 1, the near-source flow of the ‘forced’ fountain is dominated by source momentum flux and behaves like a jet; the asymptotic solution to the fountain equations yields, in agreement with previous studies, zm/b0 ~ Fr04/3. For Fr0 = O(1) the fountain is ‘weak’ and fluid is projected vertically to a height that is consistent with an energy-conserving flow – the sensitivity of the rise height with Fr0 increases as zm/b0 ~ Fr02. For Fr0 ≪ 1, the fountain is ‘very weak’ and we find that zm/b0 ~ Fr02/3. As the local value of the Froude number decreases with height, all three forms of fountain behaviour identified are expected above a highly forced source and we provide scalings for the three lengths that contribute to the total rise height. Comparisons between our predicted rise heights and the previous experimental results show good agreement across a wide range of Fr0. The collated data highlights that experiments have focused in the majority on fountains above sources with intermediate Fr0. Notably there is a lack of measurements on very weak line fountains and of independent experimental confirmation of the initial rise heights across the range of Fr0. |
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AbstractList | We present analytical solutions for the initial rise height zm of two-dimensional turbulent fountains issuing from a horizontal linear source of width 2b0 into a quiescent environment of uniform density. Using the initial rise height prediction as a measure we classify line fountains into three types depending on their source conditions. For source Froude numbers Fr0 > > 1, the near-source flow of the 'forced' fountain is dominated by source momentum flux and behaves like a jet; the asymptotic solution to the fountain equations yields, in agreement with previous studies, zm/b0 ~ Fr04/3. For Fr0 = O(1) the fountain is 'weak' and fluid is projected vertically to a height that is consistent with an energy-conserving flow - the sensitivity of the rise height with Fr0 increases as zm/b0 ~ Fr02. For Fr0 < < 1, the fountain is 'very weak' and we find that zm/b0 ~ Fr02/3. As the local value of the Froude number decreases with height, all three forms of fountain behaviour identified are expected above a highly forced source and we provide scalings for the three lengths that contribute to the total rise height. Comparisons between our predicted rise heights and the previous experimental results show good agreement across a wide range of Fr0. The collated data highlights that experiments have focused in the majority on fountains above sources with intermediate Fr0. Notably there is a lack of measurements on very weak line fountains and of independent experimental confirmation of the initial rise heights across the range of Fr0. We present analytical solutions for the initial rise height zm of two-dimensional turbulent fountains issuing from a horizontal linear source of width 2b0 into a quiescent environment of uniform density. Using the initial rise height prediction as a measure we classify line fountains into three types depending on their source conditions. For source Froude numbers Fr0 >> 1, the near-source flow of the 'forced' fountain is dominated by source momentum flux and behaves like a jet; the asymptotic solution to the fountain equations yields, in agreement with previous studies, zm/b0 ~ Fr04/3. For Fr0 = O(1) the fountain is 'weak' and fluid is projected vertically to a height that is consistent with an energy-conserving flow - the sensitivity of the rise height with Fr0 increases as zm/b0 ~ Fr02. For Fr0 << 1, the fountain is 'very weak' and we find that zm/b0 ~ Fr02/3. As the local value of the Froude number decreases with height, all three forms of fountain behaviour identified are expected above a highly forced source and we provide scalings for the three lengths that contribute to the total rise height. Comparisons between our predicted rise heights and the previous experimental results show good agreement across a wide range of Fr0. The collated data highlights that experiments have focused in the majority on fountains above sources with intermediate Fr0. Notably there is a lack of measurements on very weak line fountains and of independent experimental confirmation of the initial rise heights across the range of Fr0. [PUBLICATION ABSTRACT] We present analytical solutions for the initial rise height z m of two-dimensional turbulent fountains issuing from a horizontal linear source of width 2 b 0 into a quiescent environment of uniform density. Using the initial rise height prediction as a measure we classify line fountains into three types depending on their source conditions. For source Froude numbers Fr 0 ≫ 1, the near-source flow of the ‘forced’ fountain is dominated by source momentum flux and behaves like a jet; the asymptotic solution to the fountain equations yields, in agreement with previous studies, z m / b 0 ~ Fr 0 4/3 . For Fr 0 = O (1) the fountain is ‘weak’ and fluid is projected vertically to a height that is consistent with an energy-conserving flow – the sensitivity of the rise height with Fr 0 increases as z m / b 0 ~ Fr 0 2 . For Fr 0 ≪ 1, the fountain is ‘very weak’ and we find that z m / b 0 ~ Fr 0 2/3 . As the local value of the Froude number decreases with height, all three forms of fountain behaviour identified are expected above a highly forced source and we provide scalings for the three lengths that contribute to the total rise height. Comparisons between our predicted rise heights and the previous experimental results show good agreement across a wide range of Fr 0 . The collated data highlights that experiments have focused in the majority on fountains above sources with intermediate Fr 0 . Notably there is a lack of measurements on very weak line fountains and of independent experimental confirmation of the initial rise heights across the range of Fr 0 . We present analytical solutions for the initial rise height zm of two-dimensional turbulent fountains issuing from a horizontal linear source of width 2b0 into a quiescent environment of uniform density. Using the initial rise height prediction as a measure we classify line fountains into three types depending on their source conditions. For source Froude numbers Fr0 > > 1, the near-source flow of the 'forced' fountain is dominated by source momentum flux and behaves like a jet; the asymptotic solution to the fountain equations yields, in agreement with previous studies, zm/b0 ~ Fr04/3. For Fr0 = O(1) the fountain is 'weak' and fluid is projected vertically to a height that is consistent with an energy-conserving flow - the sensitivity of the rise height with Fr0 increases as zm/b0 ~ Fr02. For Fr0 [Lt] 1, the fountain is 'very weak' and we find that zm/b0 ~ Fr02/3. As the local value of the Froude number decreases with height, all three forms of fountain behaviour identified are expected above a highly forced source and we provide scalings for the three lengths that contribute to the total rise height. Comparisons between our predicted rise heights and the previous experimental results show good agreement across a wide range of Fr0. The collated data highlights that experiments have focused in the majority on fountains above sources with intermediate Fr0. Notably there is a lack of measurements on very weak line fountains and of independent experimental confirmation of the initial rise heights across the range of Fr0. We present analytical solutions for the initial rise height zm of two-dimensional turbulent fountains issuing from a horizontal linear source of width 2b0 into a quiescent environment of uniform density. Using the initial rise height prediction as a measure we classify line fountains into three types depending on their source conditions. For source Froude numbers Fr0 ≫ 1, the near-source flow of the ‘forced’ fountain is dominated by source momentum flux and behaves like a jet; the asymptotic solution to the fountain equations yields, in agreement with previous studies, zm/b0 ~ Fr04/3. For Fr0 = O(1) the fountain is ‘weak’ and fluid is projected vertically to a height that is consistent with an energy-conserving flow – the sensitivity of the rise height with Fr0 increases as zm/b0 ~ Fr02. For Fr0 ≪ 1, the fountain is ‘very weak’ and we find that zm/b0 ~ Fr02/3. As the local value of the Froude number decreases with height, all three forms of fountain behaviour identified are expected above a highly forced source and we provide scalings for the three lengths that contribute to the total rise height. Comparisons between our predicted rise heights and the previous experimental results show good agreement across a wide range of Fr0. The collated data highlights that experiments have focused in the majority on fountains above sources with intermediate Fr0. Notably there is a lack of measurements on very weak line fountains and of independent experimental confirmation of the initial rise heights across the range of Fr0. |
Author | HUNT, G. R. COFFEY, C. J. |
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Cites_doi | 10.1017/S0022112006009414 10.1093/petrology/30.4.885 10.1017/S0022112090002099 10.1017/S002211207700189X 10.1017/S0022112006000383 10.1017/S0022112006004435 10.1007/s003480050397 10.1061/(ASCE)0733-9399(1997)123:10(973) 10.1017/S0022112066001526 10.1017/S0022112097008252 10.1017/S0022112001003871 10.1017/S0022112008002310 10.1098/rspa.1956.0011 10.1080/104077800750022520 10.1080/00102208808924014 10.1002/9780470087923.hhs011 |
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Keywords | Turbulent flow Vertical jet Fountain Theoretical study Height Linear source Axial symmetry |
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References | S0022112008005144_ref8 Lin (S0022112008005144_ref12) 2000; 38 S0022112008005144_ref7 S0022112008005144_ref6 S0022112008005144_ref5 S0022112008005144_ref4 S0022112008005144_ref3 S0022112008005144_ref1 S0022112008005144_ref18 White (S0022112008005144_ref16) 2003 Batchelor (S0022112008005144_ref2) 1967 S0022112008005144_ref13 S0022112008005144_ref10 S0022112008005144_ref11 S0022112008005144_ref17 S0022112008005144_ref14 S0022112008005144_ref15 S0022112008005144_ref9 |
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Snippet | We present analytical solutions for the initial rise height zm of two-dimensional turbulent fountains issuing from a horizontal linear source of width 2b0 into... We present analytical solutions for the initial rise height z m of two-dimensional turbulent fountains issuing from a horizontal linear source of width 2 b 0... |
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SubjectTerms | Energy conservation Exact sciences and technology Fluid dynamics Froude number Fundamental areas of phenomenology (including applications) Jets Physics Turbulent flows, convection, and heat transfer |
Title | Characterising line fountains |
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