Enviar artigo por via de e-mail Acoustic Diagnostics of Underwater Emissions Propagating in the Form of a Multiphase Jet
- Autores: Gimaltdinov I.K.1, Stolpovsky M.V.1, Kochanova E.Y.1
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Afiliações:
- Ufa State Petroleum Technological University
- Edição: Volume 70, Nº 2 (2024)
- Páginas: 174-179
- Seção: ФИЗИЧЕСКАЯ АКУСТИКА
- URL: https://rjraap.com/0320-7919/article/view/648374
- DOI: https://doi.org/10.31857/S0320791924020047
- EDN: https://elibrary.ru/YNNBCM
- ID: 648374
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Resumo
The interaction of a pressure pulse with a gas-liquid zone, which is a section of a flooded multiphase jet consisting of a mixture of water and oil and containing a bubble core of methane, is numerically investigated. The possibility of determining the degree of expansion of the jet, the volume content of oil and gas in the jet from reflected signals is shown.
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Sobre autores
I. Gimaltdinov
Ufa State Petroleum Technological University
Autor responsável pela correspondência
Email: iljas_g@mail.ru
Rússia, Ufa
M. Stolpovsky
Ufa State Petroleum Technological University
Email: iljas_g@mail.ru
Rússia, Ufa
E. Kochanova
Ufa State Petroleum Technological University
Email: iljas_g@mail.ru
Rússia, Ufa
Bibliografia
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- Диденкулов И.Н., Кустов А.М., Мартьянов А.И., Прончатов-Рубцов Н.В. Акустическая диагностика пузырьковых объектов в жидкости // Акуст. журн. 2011. Т. 57. № 2. С. 246–251.
- Максимов А.О. Спектр шума “газового факела” // Акуст. журн. 2005. Т. 51. № 4. С. 511–519.
- Губайдуллин Д.А. Особенности отражения акустических волн от границы или слоя двухфазной среды // Акуст. журн. 2018. Т. 64. № 2. С. 162–173.
- Шагапов В.Ш., Гималтдинов И.К. Об эволюции линейных волн в жидкости при наличии пузырьковой завесы // Инженерно-физический журнал. 1998. Т. 71. № 6. С. 987–992.
- Yapa P.D., Dasanayaka L.K., Bandara U.C., Nakata K.A. Model (MEGADEEP) to simulate the transport and Fate of gas and hydrates released in deep water // Journal of hydraulic research, IAHR. 2010. V. 48. № 5. P. 559–572.
- Нигматулин Р.И. Динамика многофазных сред. Ч. 1, 2. М.: Наука, 1987. 386 с.
- Гималтдинов И.К., Кочанова Е.Ю. Условия фокусировки волны давления в пузырьковом клине // Акуст. журн. 2020. Т. 66. № 4. С. 351–356.
- Ильгамов М.А., Гильманов А.Н. Неотражающие условия на границах расчетной области. М.: Физматлит, 2003. 240 с.
- Исакович М.А. Общая акустика. Учебное пособие. М.: Наука, 1973. 502 с.
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Fig. 1. Schematic representation of the computational domain. D1–D6 – pressure sensors
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Fig. 2. Pressure diagrams at moments (a) - 1.62 ms, (b) - 2.5 ms, (c) – 3.5 ms. Calculation parameters: liquid – in the gas-liquid zone: a mixture of oil and water with volume contents ao0 = 0.75 and aw0 = 0.25, methane gas: ag0 = 0.001, a = 1.25 mm, x1 = 2.95 m, x2 = 3.05 m, x2l = 3.3 m, x1l = 2.7 m, x2g = 3.2 m, x1g = 2.8 m, ∆pl0 = 0.5 MPa, po00 = 830 kg/m3, pw00 = 1000 kg/m3,vo = 10-2 m2/s, vw = 10-6 m2/s, Co = 1225 m/s, Cw = 1500 m/s, pg00 = 50.19 kg/m3, cg = 2220 J/kg K, λg = 0.03 W/m K, T0 = 300 K, p0 = 7.0 MPa
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Fig. 3. Waveforms for sensors D3, D2, D1 having coordinates (2;2), (2;1) and (2;0) m, the letters r1 and r2 indicate the signals reflected from the boundaries “water–oil–water mixture-gas-liquid core” and “gas-liquid core-oil-water mixture- water.” All parameters are the same as for Fig. 2
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Fig. 4. Velocity field at 2.8 ms. The volume content of the gas is ag0 = 0.01.The other parameters are the same as in Fig. 2
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Fig. 5. Waveforms of reflected signals for the D3 sensor: bold lines correspond to the volume content of gas in the bubble core (a) – ag0 = 0.001 and (b) – ag0 = 0.01, thin lines correspond to the case of the absence of a bubble core in the jet (ag0 = 0). Volume content of oil and gas in the area of a multiphase jet: ao0 = 0.75, aw0 = 0.25. The other parameters are the same as in Fig. 2
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Fig. 6. The same as in Fig. 5. The bold line in both pictures corresponds to the case when the volume fraction of oil in the liquid phase of the bubble zone is ao0 = 0.75 (aw0 = 0.25), the thin one is ao0 = 0.25 (aw0 = 0.75). The volume content of the gas is (a) – ag0 = 0.001, (b) – ag0 = 0.01. The other parameters are the same as in Fig. 2
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