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1.
Modifications of integral bubble and jet models including the pressure force are proposed. Exact solutions are found for the modified model of a stationary convective jet from a point source of buoyancy and momentum. The exact solutions are compared against analytical solutions of the integral models for a stationary jet that are based on the approximation of the vertical boundary layer. It is found that the modified integral models of convective jets retain the power-law dependences on the altitude for the vertical velocity and buoyancy obtained in classical models. For a buoyant jet in a neutrally stratified atmosphere, the inclusion of the pressure force increases the amplitude of buoyancy and decreases the amplitude of vertical velocity. The total amplitude change is about 10%. It is shown that in this model there is a dynamic invariant expressing the law of a uniform distribution of the potential and kinetic energy along the jet axis. For a spontaneous jet rising in an unstably stratified atmosphere, the inclusion of the pressure force retains the amplitude of buoyancy and increases the amplitude of vertical velocity by about 15%. It is shown that in the model of a spontaneous jet there is a dynamic invariant expressing the law of a uniform distribution of the available potential and kinetic energy along the jet axis. The results are of interest for the problems of anthropogenic pollution diffusion in the air and water environments and the formulation of models for statistical and stochastic ensembles of thermals in a mass-flux parameterization of turbulent moments. 相似文献
2.
A comprehensive numerical study on the three-dimensional structure of a turbulent jet in crossflow is performed. Thejet-to-crossflow velocity ratio (R) varies in the range of 2 ～ 16; both vertical jets and inclined jets without excess streamwisemomentum are considered. The numerical results of the standard two-equation k-~ model show that the turbulent structurecan be broadly categorised according to the jet-to-crossflow velocity ratio. For strong to moderate jet discharges, i.e. R >4, the jet is characterized by a longitudinal transition through a bent-over phase during which the jet becomes almost parallelwith the main freestream, to a sectional vortex-pair flow with double concentration maxima; the computed flow details andscalar mixing characteristics can be described by self-similar relations beyond a dimensionless distance of around 20 ～ 60.The similarity coefficients are only weakly dependent on R. The cross-section scalar field is kidney-shaped and bifurcated,with distinct double concentration maxima; the aspect ratio is found to be around 1.2. A loss in vertical momentum is ob-served and the added mass coefficient of the jet motion is found to be approximately 1. On the other hand, for weak jets instrong crossflow, i.e. R≤ 2, the lee of the jet is characterized by a negative pressure region. Although the double vortexflow can still be noted, the scalar field becomes more symmetrical and no longer bifurcated. The similarity coeffcients are al-so noticeably different. The predicted jet flow characteristics and mixing rates are well supported by experimental and field data 相似文献
3.
Compact zero-mass pulsatile jet actuators are proposed for low-speed maneuvering and station keeping of small underwater vehicles.1 The flow field of such jets are initially dominated by vortex ring formation. Pinched-off vortices characterize the extremum impulse accumulated by the leading vortex ring in a vortex ring formation process. Relevant parameters in this process are identified in order to design simple and low cost zero-mass pulsatile jet actuators. Thrust optimization of synthetic jets for maximal thrust generation is achieved by enforcing the jet formation number to be around 4. Prototypes of such actuators are built and tested for underwater maneuvering and propulsion. The actuators could be used in two ways: (i) to improve the low-speed maneuvering and station keeping capabilities of traditional propeller driven underwater vehicles, and (ii) as a synthetic jet for flow control and drag reduction at higher cruising speeds. A model for calculating the rotation rate of the underwater vehicle is also proposed and verified. 相似文献
4.
The basic properties of the dynamic model of a turbulent jet formed by a deep-water sewage discharge into the stratified environment of coastal regions are considered. The model developed was used to estimate the parameters of a floating-up jet of deep wastewater discharge from Sand Island into the basin of Mamala Bay (Hawaii) depending on the season and discharge operation mode. The estimates of the float-up depths of the jet and the initial dilution of the jet were estimated on the basis of model calculations using experimental data on the vertical profiles of the water temperature and salinity under the actual conditions of stratification in the study region. It is shown that the further propagation of the wastewater jet depends on tidal events and internal waves generated by tides. The appearance of turbulent jets at the sea surface was recorded. The model estimates of the parameters of the wastewater discharge were compared with the results of experimental measurements. Good agreement was found, which indicates that the physical mechanisms of the propagation of turbulent jets in a stratified medium are adequately described by the model. 相似文献
5.
采用激光诱导荧光技术(laser induced fluorescence-LIF)对同向流动环境中具有不同喷口高宽比(aspect ratio-AR)、射流比(velocity ratio-VR)的椭圆喷口射流与圆喷口射流的标量物质浓度场进行可视化和定量化研究。系统研究了同向流动环境中椭圆喷口射流浓度场的各种掺混稀释特性:中心线稀释度,射流扩展宽度,下游不同断面上的时均浓度分布和紊动强度分布。采用紊流理论和量纲分析方法对实验数据进行分析讨论,给出同向流动环境中受动量控制的椭圆射流稀释度预报方法,提出该类椭圆射流稀释度预报方法归并到已有圆射流系列预报模型中的实现途径,比较了具有相同出口超值动量Me0的圆射流与椭圆射流的沿程稀释度变化。由于椭圆射流比圆射流具有更高的稀释度增长比率,说明椭圆射流比圆射流具有更好的掺混稀释效果。 相似文献
6.
Application of the standard Eulerian model to simulations of sand scour results in unrealistic phenomena. Therefore, the present work develops a modified Eulerian model based on sand incipient motion theory. The modified model is applied for simulating a two-dimensional single vertical jet and a moving planar jet. The simulation results generally demonstrate fairly good agreement with published results of scour profiles and the velocity contours of the water and sand phases. In addition, equations to describe self-similar scour profiles for the moving planar jet cases are given. The results demonstrate that the modified model efficiently and accurately simulates the two-dimensional sand scour produced by jets, particularly for the moving jet cases. 相似文献
7.
L. Kh. Ingel 《Izvestiya Atmospheric and Oceanic Physics》2016,52(6):602-605
In traditional theoretical models of convection from isolated sources, results usually depend little on their sizes: convective jets and isolated thermals rapidly “forget” the source geometry. However, new problems in which the sizes of a source are relatively large and can significantly influence results have recently become important. These are, for example, problems of the dynamics of intensive methane emissions of geologic origin. The paper generalizes some well-known integral models of thermals and jets. Although these simple schemes cannot compete with complicated numerical models in describing the spatial structure of the currents, they are shown to be able to reproduce a number of important numerical results rather well (the height and time of the rise of convective elements) and, moreover, to find clear physical laws and determine explicit dependences on parameters of the problem. 相似文献
8.
An ensemble of convective thermals is distinguished from the surface layer of penetrative turbulent convection over a heated horizontally uniform surface. A statistical model of the ensemble of convective thermals is developed that uses the idea of entropy in the Boltzmann-Jaynes form. The distribution of thermals by potential energies is shown to display an entropy maximum. On the basis of the Boltzmann distribution by potential energies, the temperature distribution of spontaneous jets is obtained and found to be consistent with known experimental data. 相似文献
9.
为研究风急流对吕宋海峡处黑潮路径的影响,本文使用1.5层约化重力浅水模式,设置了与吕宋海峡跨度相接近的缺口宽度,考虑西边界流在西边界缺口处当处于迟滞过程的临界状态时,其路径受风急流影响的动力机制,并初步探讨了在实际海陆边界条件下,实际风急流对黑潮路径的影响。结果显示,理想情况下,当西边界流处在由入侵流态到跨隙流态转变的临界状态时,西风、南风以及西南风风急流可以激发西边界流由入侵流态转变为跨隙流态。当西边界流处在由跨隙流态向入侵流态转变的临界状态时,北风、东风以及东北风风急流可以激发西边界流由跨隙流态转变为入侵流态,并且在风急流消失后西边界流不能再恢复到初始流态。实际情况下,冬季风急流有利于黑潮入侵南海,夏季风急流有利于黑潮跨越吕宋海峡,这和理想情况下的模拟结果以及实际观测结果相一致,这对进一步研究南海北部的上层环流以及南海的质量、能量输送有重要意义。 相似文献
10.
Reverse tip jets are strong low-level winds with easterly component that form near the southern tip of Greenland. In the present study, a reverse tip jet case which occurred from 21 to 22 December 2000 was examined to clarify its fine structure using a numerical model with a horizontal resolution of 3 km. The reverse tip jet, showing the supergeostrophic wind speed with a maximum wind speed in excess of 45 m s−1 , extended from the east coast of Greenland to the west of Cape Farewell with anticyclonic curvature. A cloud free region coincided with the jet indicated that there was a mesoscale downdraft. Along the eastern edge of the jet, a banded cloud formed between the upstream easterly wind and the colder northerly wind that is a part of the jet and is located along the east coast. This cloud was associated with large gradients in surface wind speed, temperature, moisture, and heat flux. A maximum surface total heat flux of 300 W m−2 coincided with the location of the jet. It is suggested that the orographic deflection by Greenland's large-scale topography as well as small-scale downslope winds behind mountains with fiords causes the reverse tip jet. 相似文献
11.
V. G. Bondur Yu. V. Grebenyuk E. V. Ezhova V. I. Kazakov D. A. Sergeev I. A. Soustova Yu. I. Troitskaya 《Izvestiya Atmospheric and Oceanic Physics》2009,45(6):779-790
In a large test reservoir with artificial temperature stratification at the Institute of Applied Physics, Russian Academy
of Sciences, we have performed a major laboratory simulation of the nonstationary dynamics of buoyant turbulent jets generated
by wastewater flows from underwater collector diffusers. The interaction of buoyant jets with the pycnocline leads to an active
generation of internal waves. An analysis of the dependence of wave amplitude on the control parameter proportional to the
rate of liquid flow from the collector diffuser has indicated that this dependence is adequately described by a function that
is characteristic for the presence in the Hopf bifurcation system, which occurs for a soft actuation mode of self-oscillations
of the globally instable mode. To check the conditions for the actuation of the globally instable mode, we have performed
an auxiliary experiment in a small reservoir with a salt stratification formulated similar to the experiment in the big reservoir.
Using the particle image velocimetry (PIV) method, we have measured the velocity field in the buoyant jet and constructed
the profiles of transverse velocity in several sections. When the jet approaches the pycnocline, a counterflow is generated
at the edges. A stability analysis for the resulting profiles of flow velocities performed by the method of normal modes has
revealed that, for the jet portions with counterflow, the condition of absolute instability by the Briggs criterion for axisymmetric
jet oscillations is satisfied, which testifies to the fact that the globally instable mode is actuated. The estimates for
oscillation frequencies of the globally instable mode are well consistent quantitatively with the measured spectrum of jet
oscillations. 相似文献
12.
A static experimental system based on the background of the underwater gun firing process is designed to simulate the expansion of conical-distributed multiple gas jets in a water-filled vessel. The gas is generated from the gunpowder combustion and injected into water through five orifices on a mock bullet. A high-speed digital camera is taken in experiment to record such expansion and the Euler-Euler multiphase model is utilized in simulation to describe the gas-liquid flow. Results show that the contraction of Taylor cavity in liquid and the gas-liquid entrainment both affect the shock structure in gas. The expansion zone near the orifice shrinks and the gas speed downs when the central gas jet has a contraction, but lateral jets have no contractions due to the obstruction from the wall. The contraction has a greater impact on the shock structure than the gas-liquid entrainment and occurs earlier under a higher injection pressure. 相似文献
13.
The flow characteristics of tidal jets induced by a Tidal-Jet Generator (TJG) are investigated using a finite-difference numerical scheme, named Navier–Stokes (NS)–Marker and Cell (MAC)-TIDE, based on the fully 3D NS equations. The TJG is an enclosed rectangular breakwater, which has vertical opening and a large enclosed volume inside. During both phases of tide, strong and uni-directional jets can be obtained locally from the inlet of the TJG, due to the water level difference between the inner and outer sides of TJG.The computed results are extensively compared with three other independently developed numerical models; 3D-ADI, DVM, and CIP-CSF. These models are based on quasi-3D, 2D depth-averaged, and fully 3D NS equations, respectively. It is seen that the present fully 3D numerical model NS–MAC-TIDE can predict the maximum intensity of inlet velocity with higher accuracy than the other numerical models when compared with the empirical function proposed from the experiments. The numerical simulations based on NS–MAC-TIDE can reproduce successfully the processes of generation, development, and dissipation of tidal jets. The effects of gap opening on the main characteristics of the tidal jet flow are assessed. Through numerical assessment, it is also clearly demonstrated that the residual time of a pollutant distributed around the front of the TJG can be decreased by significant amount due to the locally induced tidal jet. The TJG can thus utilize tidal energy for water purification in local marine environment by providing a flushing mechanism. 相似文献
14.
Both wind turning with height and ageostrophic flow in a stably stratified atmospheric boundary layer are analyzed using a three-parameter turbulence model. For a quasi-steady state of the boundary layer, the cross-isobaric flow is determined only by turbulent stress at the surface in the direction of geostrophic wind. The “operative” prediction models, in which the first-order turbulence closure schemes are used, tend to overestimate the boundary-layer depth and underestimate the angle between the surface and geostrophic winds when compared to “research” models (schemes of high-level turbulence closure). The true value of the angle between the surface and geostrophic winds is significant for the presentation of a large-scale flow. A nocturnal low-level jet is a mesoscale phenomenon reflected in data obtained from measurements in a stably stratified atmospheric boundary layer. It is found that such jets are of great importance in transporting humidity, momentum, and air pollution. In this study, the difference between jet flows over a homogeneous underlying surface and over a spatially localized large-scale aerodynamic roughness is shown. 相似文献
15.
V. I. Bukreev 《Oceanology》2013,53(1):110-118
A technique and some results of laboratory experiments, in which the densification during mixing of the salt water masses with the same initial densities occurs, are presented. A graphical interpretation of the densification during mixing and an empirical formula describing the dependence of the water density on temperature and concentration of the dissolved salt NaCl at atmospheric pressure are given. Examples of spreading of the initially horizontal, inclined and vertical round jets as well as a vertical plane jet are considered. In all examples, the jet submerged up to the bottom of the experimental setup. It was found that the submergence velocity was on the order of 0.5 ± 0.1 cm/s. The influence of the double diffusion on the jet submergence velocity in the salt water is discussed. 相似文献
16.
We present a case study of low-level wind jets induced in sequence by orographic effects off the Pacific coast of northern
Japan during 7–11 June 2003, and demonstrate that the transition of the wind jets causes areal differences of wave height
variations along the coast. First, we describe evolution and structure of the wind jet by analyzing SeaWinds scatterometer
wind measurements. Under the easterly wind, a strong wind jet formed after passing by Cape Erimo. As the wind shifted to the
southeast, the wind jet started to decay. In turn, the southerly wind along the coast led to another wind jet in the lee of
the easternmost tip of the Sanriku coast. We then identify onsets and decays of the wind jets from time series of wind speed
at meteorological stations. Finally, we demonstrate that the transition of the wind jets has local impacts on wave height
variations. Significant wave heights measured by altimeters were correlated positively with local wind energy, i.e., squares
of wind speeds. Accompanying the wind jet formation/decline, significant differences of wave height variations became marked
among wave observation stations located along the coast at intervals of up to 50 km. 相似文献
17.
A coupled ocean-ice-wave model is used to study ice-edge jet and eddy genesis during surface gravity wave dissipation in a frazil-pancake ice zone. With observational data from the Beaufort Sea, possible wave dissipation processes are evaluated using sensitivity experiments. As wave energy dissipated, energy was transferred into ice floe through radiation stress. Later, energy was in turn transferred into current through ocean-ice interfacial stress. Since most of the wave energy is dissipated at the ice edge, ice-edge jets, which contained strong horizontal shear, appeared both in the ice zone and the ocean. Meanwhile, the wave propagation direction determines the velocity partition in the along-ice-edge and cross-ice-edge directions, which in turn determines the strength of the along-ice-edge jet and cross-ice-edge velocity. The momentum applied in the along-ice-edge(cross-ice-edge)direction increased(decreased) with larger incident angle, which is favorable condition for producing stronger mesoscale eddies, vice versa. The dissipation rate increases(decreases) with larger(smaller) wavenumber, which enhances(reduces) the jet strength and the strength of the mesoscale eddy. The strong along-ice-edge jet may extend to a deep layer(> 200 m). If the water depth is too shallow(e.g., 80 m), the jet may be largely dampened by bottom drag, and no visible mesoscale eddies are found. The results suggest that the bathymetry and incident wavenumber(magnitude and propagation direction) are important for wave-driven current and mesoscale eddy genesis. 相似文献
18.
The eruption of an underwater volcano can initiate the disturbances of the sea surface and subsequently generate a group of outward-propagating tsunamis. The theme of this study is to introduce a three-dimensional (3D) fully nonlinear wave model for the simulation of wave motions induced by a bottom jet. A boundary-fitted coordinate system is utilized to conveniently adjust grids according to the transient moving free surface. The governing Laplace equation of the velocity potential is solved by an implicit finite-difference scheme while a mixed explicit/implicit iteration procedure is applied to solve the free-surface boundary conditions. In addition, a set of generalized Boussinesq equations are solved for comparison with the fully nonlinear model. Good agreements in comparisons with the existing numerical and analytical solutions are achieved for cases investigated. Waves induced by three types of bottom jets: namely (1) sudden eruption, (2) initial transient, and (3) periodic transient are discussed in this paper. For the case of sudden erupted jet, a system of 3D outgoing waves as the cylindrical wave pattern are presented and discussed. For the initial transient types, it shows the transition in the incipient stage has a great influence on the initial rising of the water surface and the induced leading waves. Furthermore, an interesting up-down phenomenon in the center of disturbed free surface due to the type of periodic jet is revealed. 相似文献
19.
为深入研究井喷和管道破损等海底事故后溢油在水下环境中的输移扩散过程，文章利用自制的组合式环形水槽（周长9.7 m、宽0.45 m、深1 m），以阿曼原油与消油剂混合物和淡水（含示踪剂）为模拟污染物，初步开展静水和动水环境中海底溢油浮射流的物理模拟实验，并应用基于拉格朗日积分方法的水下溢油浮射流模型进行数值模拟比较分析。研究结果表明:静水环境中，水下溢油浮射流主要沿喷口的垂直中心线向水面输移扩散；非均匀流动水环境中，横流速度越大，浮射流输移轨迹的弯曲程度越明显；数值模拟的浮射流轨迹总体上与实验观测结果符合较好；研究结果可为今后相关物理实验和数值模型的改进研究提供有益参考。 相似文献
20.
E. V. Ezhova D. A. Sergeev A. A. Kandaurov Yu. I. Troitskaya 《Izvestiya Atmospheric and Oceanic Physics》2012,48(4):409-417
The nonsteady dynamics of turbulent axially symmetrical jets in stratified fluid with a great density gradient (pycnocline) is studied in laboratory experiments in the large test reservoir with artificial temperature stratification at the Institute of Applied Physics, Russian Academy of Sciences (IAP RAS) simulating wastewater flows from underwater collectors in coastal cities. An underwater survey of jets in the pycnocline region has been carried out along with synchronous measurements of internal waves. It is shown that a jet quasiperiodically oscillates in a vertical plane, thus effectively generating internal waves when interacting with the pycnocline. It is ascertained that the axially symmetrical mode of jet oscillations is a source of internal waves. 相似文献