{"title":"计算重力流瞬时体积的数学模型:以意外释放的混合机制和体积增长为重点的实验分析","authors":"Raphael R.C. Santos, Sávio S.V. Vianna","doi":"10.1016/j.jlp.2024.105354","DOIUrl":null,"url":null,"abstract":"<div><p>We present experiments of two dimensional high-Reynolds (<span><math><mrow><mi>R</mi><mi>e</mi><mo>></mo><mn>2400</mn></mrow></math></span>) turbulent gravity current advancing down on slope <span><math><mrow><mo>(</mo><mi>θ</mi><mo>=</mo><mn>5</mn><mo>°</mo><mo>)</mo></mrow></math></span> generated by continuous buoyancy flux. The current research is focused on understanding the flow mixing mechanism and consequently the rate of volume growth for the development of mathematical model to calculate the volume of the current. The gravity currents were obtained pumping saline solution continuously into a channel filled with fresh water. Images of the flow were taken with a ratio of 4 frames per second (fps). The gravity current buoyancy distribution was obtained by using light attenuation technique to calculate the cross-channel average of the density. It was found that the proportional parameter <span><math><mi>λ</mi></math></span> in <span><math><mrow><msub><mrow><mi>U</mi></mrow><mrow><mi>F</mi></mrow></msub><mo>=</mo><mi>λ</mi><msup><mrow><mrow><mo>(</mo><msub><mrow><mi>Q</mi></mrow><mrow><mn>0</mn></mrow></msub><msubsup><mrow><mi>g</mi></mrow><mrow><mn>0</mn></mrow><mrow><mo>′</mo></mrow></msubsup><mo>)</mo></mrow></mrow><mrow><mn>1</mn><mo>/</mo><mn>3</mn></mrow></msup></mrow></math></span> is <span><math><mrow><mi>λ</mi><mo>=</mo><mn>1</mn><mo>.</mo><mn>23</mn><mo>/</mo><mi>F</mi><msubsup><mrow><mi>r</mi></mrow><mrow><mn>0</mn></mrow><mrow><mn>1</mn><mo>/</mo><mn>12</mn></mrow></msubsup></mrow></math></span>. The head reaches a dynamic equilibrium for <span><math><mrow><mi>F</mi><msub><mrow><mi>r</mi></mrow><mrow><mi>F</mi></mrow></msub><mo>≈</mo><mn>0</mn><mo>.</mo><mn>95</mn></mrow></math></span>, where <span><math><mrow><mi>F</mi><msub><mrow><mi>r</mi></mrow><mrow><mi>H</mi></mrow></msub><mo>=</mo><msub><mrow><mi>U</mi></mrow><mrow><mi>F</mi></mrow></msub><mo>/</mo><msqrt><mrow><msubsup><mrow><mi>g</mi></mrow><mrow><mi>F</mi></mrow><mrow><mo>′</mo></mrow></msubsup><msub><mrow><mi>h</mi></mrow><mrow><mi>F</mi></mrow></msub></mrow></msqrt></mrow></math></span>. Three mixing zones were observed; near the source, tail and head. The ambient fluid volume fluxes entraining the current into this three zones were modelled in terms of entrainment coefficients <span><math><msub><mrow><mi>ɛ</mi></mrow><mrow><mi>j</mi></mrow></msub></math></span>, <span><math><msub><mrow><mi>ɛ</mi></mrow><mrow><mi>T</mi></mrow></msub></math></span>, <span><math><msub><mrow><mi>ɛ</mi></mrow><mrow><mi>H</mi></mrow></msub></math></span>, respectively. A model of the rate of growth of the volume of the current was developed, it is written as <span><math><mrow><mi>d</mi><mi>V</mi><mo>/</mo><mi>d</mi><mi>t</mi><mo>=</mo><msub><mrow><mi>Q</mi></mrow><mrow><mn>0</mn></mrow></msub><mrow><mo>(</mo><mn>1</mn><mo>+</mo><msub><mrow><mi>ɛ</mi></mrow><mrow><mi>J</mi></mrow></msub><mo>)</mo></mrow><mo>/</mo><mrow><mo>(</mo><mn>1</mn><mo>−</mo><msup><mrow><mi>λ</mi></mrow><mrow><mn>3</mn></mrow></msup><msub><mrow><mi>ɛ</mi></mrow><mrow><mi>H</mi></mrow></msub><mo>)</mo></mrow></mrow></math></span>. One of the simplifications implies that the volume growth rate is constant. Good agreement with experimental data is observed.</p></div>","PeriodicalId":16291,"journal":{"name":"Journal of Loss Prevention in The Process Industries","volume":null,"pages":null},"PeriodicalIF":3.6000,"publicationDate":"2024-05-24","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"A mathematical model for calculating the transient volume of gravity currents: An experimental analysis focused on mixing mechanisms and volume growth for accidental releases\",\"authors\":\"Raphael R.C. Santos, Sávio S.V. Vianna\",\"doi\":\"10.1016/j.jlp.2024.105354\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><p>We present experiments of two dimensional high-Reynolds (<span><math><mrow><mi>R</mi><mi>e</mi><mo>></mo><mn>2400</mn></mrow></math></span>) turbulent gravity current advancing down on slope <span><math><mrow><mo>(</mo><mi>θ</mi><mo>=</mo><mn>5</mn><mo>°</mo><mo>)</mo></mrow></math></span> generated by continuous buoyancy flux. The current research is focused on understanding the flow mixing mechanism and consequently the rate of volume growth for the development of mathematical model to calculate the volume of the current. The gravity currents were obtained pumping saline solution continuously into a channel filled with fresh water. Images of the flow were taken with a ratio of 4 frames per second (fps). The gravity current buoyancy distribution was obtained by using light attenuation technique to calculate the cross-channel average of the density. It was found that the proportional parameter <span><math><mi>λ</mi></math></span> in <span><math><mrow><msub><mrow><mi>U</mi></mrow><mrow><mi>F</mi></mrow></msub><mo>=</mo><mi>λ</mi><msup><mrow><mrow><mo>(</mo><msub><mrow><mi>Q</mi></mrow><mrow><mn>0</mn></mrow></msub><msubsup><mrow><mi>g</mi></mrow><mrow><mn>0</mn></mrow><mrow><mo>′</mo></mrow></msubsup><mo>)</mo></mrow></mrow><mrow><mn>1</mn><mo>/</mo><mn>3</mn></mrow></msup></mrow></math></span> is <span><math><mrow><mi>λ</mi><mo>=</mo><mn>1</mn><mo>.</mo><mn>23</mn><mo>/</mo><mi>F</mi><msubsup><mrow><mi>r</mi></mrow><mrow><mn>0</mn></mrow><mrow><mn>1</mn><mo>/</mo><mn>12</mn></mrow></msubsup></mrow></math></span>. The head reaches a dynamic equilibrium for <span><math><mrow><mi>F</mi><msub><mrow><mi>r</mi></mrow><mrow><mi>F</mi></mrow></msub><mo>≈</mo><mn>0</mn><mo>.</mo><mn>95</mn></mrow></math></span>, where <span><math><mrow><mi>F</mi><msub><mrow><mi>r</mi></mrow><mrow><mi>H</mi></mrow></msub><mo>=</mo><msub><mrow><mi>U</mi></mrow><mrow><mi>F</mi></mrow></msub><mo>/</mo><msqrt><mrow><msubsup><mrow><mi>g</mi></mrow><mrow><mi>F</mi></mrow><mrow><mo>′</mo></mrow></msubsup><msub><mrow><mi>h</mi></mrow><mrow><mi>F</mi></mrow></msub></mrow></msqrt></mrow></math></span>. Three mixing zones were observed; near the source, tail and head. The ambient fluid volume fluxes entraining the current into this three zones were modelled in terms of entrainment coefficients <span><math><msub><mrow><mi>ɛ</mi></mrow><mrow><mi>j</mi></mrow></msub></math></span>, <span><math><msub><mrow><mi>ɛ</mi></mrow><mrow><mi>T</mi></mrow></msub></math></span>, <span><math><msub><mrow><mi>ɛ</mi></mrow><mrow><mi>H</mi></mrow></msub></math></span>, respectively. A model of the rate of growth of the volume of the current was developed, it is written as <span><math><mrow><mi>d</mi><mi>V</mi><mo>/</mo><mi>d</mi><mi>t</mi><mo>=</mo><msub><mrow><mi>Q</mi></mrow><mrow><mn>0</mn></mrow></msub><mrow><mo>(</mo><mn>1</mn><mo>+</mo><msub><mrow><mi>ɛ</mi></mrow><mrow><mi>J</mi></mrow></msub><mo>)</mo></mrow><mo>/</mo><mrow><mo>(</mo><mn>1</mn><mo>−</mo><msup><mrow><mi>λ</mi></mrow><mrow><mn>3</mn></mrow></msup><msub><mrow><mi>ɛ</mi></mrow><mrow><mi>H</mi></mrow></msub><mo>)</mo></mrow></mrow></math></span>. One of the simplifications implies that the volume growth rate is constant. Good agreement with experimental data is observed.</p></div>\",\"PeriodicalId\":16291,\"journal\":{\"name\":\"Journal of Loss Prevention in The Process Industries\",\"volume\":null,\"pages\":null},\"PeriodicalIF\":3.6000,\"publicationDate\":\"2024-05-24\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Journal of Loss Prevention in The Process Industries\",\"FirstCategoryId\":\"5\",\"ListUrlMain\":\"https://www.sciencedirect.com/science/article/pii/S0950423024001128\",\"RegionNum\":3,\"RegionCategory\":\"工程技术\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q2\",\"JCRName\":\"ENGINEERING, CHEMICAL\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of Loss Prevention in The Process Industries","FirstCategoryId":"5","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S0950423024001128","RegionNum":3,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"ENGINEERING, CHEMICAL","Score":null,"Total":0}
A mathematical model for calculating the transient volume of gravity currents: An experimental analysis focused on mixing mechanisms and volume growth for accidental releases
We present experiments of two dimensional high-Reynolds () turbulent gravity current advancing down on slope generated by continuous buoyancy flux. The current research is focused on understanding the flow mixing mechanism and consequently the rate of volume growth for the development of mathematical model to calculate the volume of the current. The gravity currents were obtained pumping saline solution continuously into a channel filled with fresh water. Images of the flow were taken with a ratio of 4 frames per second (fps). The gravity current buoyancy distribution was obtained by using light attenuation technique to calculate the cross-channel average of the density. It was found that the proportional parameter in is . The head reaches a dynamic equilibrium for , where . Three mixing zones were observed; near the source, tail and head. The ambient fluid volume fluxes entraining the current into this three zones were modelled in terms of entrainment coefficients , , , respectively. A model of the rate of growth of the volume of the current was developed, it is written as . One of the simplifications implies that the volume growth rate is constant. Good agreement with experimental data is observed.
期刊介绍:
The broad scope of the journal is process safety. Process safety is defined as the prevention and mitigation of process-related injuries and damage arising from process incidents involving fire, explosion and toxic release. Such undesired events occur in the process industries during the use, storage, manufacture, handling, and transportation of highly hazardous chemicals.