標(biāo)題: Titlebook: Advances in Turbulence XII; Proceedings of the 1 Bruno Eckhardt Conference proceedings 20091st edition Springer-Verlag Berlin Heidelberg 20 [打印本頁(yè)] 作者: DUBIT 時(shí)間: 2025-3-21 16:26
書目名稱Advances in Turbulence XII影響因子(影響力)
書目名稱Advances in Turbulence XII影響因子(影響力)學(xué)科排名
書目名稱Advances in Turbulence XII網(wǎng)絡(luò)公開(kāi)度
書目名稱Advances in Turbulence XII網(wǎng)絡(luò)公開(kāi)度學(xué)科排名
書目名稱Advances in Turbulence XII被引頻次
書目名稱Advances in Turbulence XII被引頻次學(xué)科排名
書目名稱Advances in Turbulence XII年度引用
書目名稱Advances in Turbulence XII年度引用學(xué)科排名
書目名稱Advances in Turbulence XII讀者反饋
書目名稱Advances in Turbulence XII讀者反饋學(xué)科排名
作者: minimal 時(shí)間: 2025-3-21 20:58
Measurement of Lagrangian Particle Trajectories by Digital in-line Holographyto filter out speckles and to enhance accuracy of the longitudinal particle coordinates. In first measurements particle trajectories were measured and visualized together with fitted spline curves. A pronounced decrease of the standard deviation of the particle coordinates with respect to their spline curves was achieved.作者: BOOM 時(shí)間: 2025-3-22 02:51
https://doi.org/10.1007/978-3-319-99414-7processes. For instance, predicting the time of rain initiation of warm clouds, which are known to be turbulent in their core, is still an open problem. Droplets in such clouds, which can be treated as inertial particles, are believed to grow to rain drop by coalescence due to collisions.作者: Hamper 時(shí)間: 2025-3-22 08:06
Introduction to Conformance Checkingto filter out speckles and to enhance accuracy of the longitudinal particle coordinates. In first measurements particle trajectories were measured and visualized together with fitted spline curves. A pronounced decrease of the standard deviation of the particle coordinates with respect to their spline curves was achieved.作者: Acclaim 時(shí)間: 2025-3-22 10:07 作者: 主講人 時(shí)間: 2025-3-22 16:13
978-3-662-51932-5Springer-Verlag Berlin Heidelberg 2009作者: ALERT 時(shí)間: 2025-3-22 18:38
Bruno EckhardtProceedings of the conference Advances in Turbulence XII.Provide useful information to researchers and graduate students.Includes supplementary material: 作者: Anecdote 時(shí)間: 2025-3-23 00:44
http://image.papertrans.cn/a/image/150054.jpg作者: 托運(yùn) 時(shí)間: 2025-3-23 01:48
Parisa Hariri,Riku Klén,Matti Vuorinental techniques allow to investigate particles with different physical properties, e.g. values of size and density, within some specific range. No experimental studies have been able to cover large range of parameters space. We have recently performed a set of Direct Numerical Simulation (DNS) with t作者: 無(wú)聊的人 時(shí)間: 2025-3-23 06:18
Springer Monographs in Mathematicsngian description of fluid turbulence and poses long standing questions on modeling of hydrodynamical forces on objects in unsteady nonuniform flows [1]. Even in the simplest conditions of highly diluted suspensions of particles whose sizes are smaller than the dissipative scale of the carrier flow,作者: Immobilize 時(shí)間: 2025-3-23 11:16 作者: Cuisine 時(shí)間: 2025-3-23 16:24 作者: certain 時(shí)間: 2025-3-23 20:56 作者: NAV 時(shí)間: 2025-3-24 02:05 作者: 聽(tīng)覺(jué) 時(shí)間: 2025-3-24 05:52 作者: 編輯才信任 時(shí)間: 2025-3-24 09:59 作者: 或者發(fā)神韻 時(shí)間: 2025-3-24 11:58
Introduction to Conformance Checkingto filter out speckles and to enhance accuracy of the longitudinal particle coordinates. In first measurements particle trajectories were measured and visualized together with fitted spline curves. A pronounced decrease of the standard deviation of the particle coordinates with respect to their spli作者: PARA 時(shí)間: 2025-3-24 17:57
Handling Noise and Incompleteness the main objections is the higher tracer density necessary for gaseous measurements [1, 2], resulting from higher characteristic speeds and smaller spaceand time-scales of the important flow structures. Nevertheless, the widely recognized interest of Lagrange-based measurements (such as PTV) for th作者: 賠償 時(shí)間: 2025-3-24 22:13
Handling non-Fitness in PracticeThe final goal of this two-particle dispersion problem is to describe the probability density function (PDF) of the dispersion .(.), which gives probability to have a pair of particles whose relative distance is . at time .. L.F. Richardson made the first attempt to phenomenologically derive an equa作者: obsolete 時(shí)間: 2025-3-25 01:21
Conformance Checking and its Challengesical flows. Pearson .. [5] used a Langevin model to predict that the mean square of vertical fluid particle displacements reaches a plateau with . in stationary stratified flows. Here, . is the vertical velocity fluctuation and N is the Brunt-V?is?l? frequency. At long times, they predict that ., wh作者: anatomical 時(shí)間: 2025-3-25 05:31 作者: Chameleon 時(shí)間: 2025-3-25 07:37 作者: inspiration 時(shí)間: 2025-3-25 14:23 作者: 6Applepolish 時(shí)間: 2025-3-25 16:15 作者: cortisol 時(shí)間: 2025-3-25 23:52 作者: Hypomania 時(shí)間: 2025-3-26 01:09
Springer Monographs in Mathematicsmple dynamical particle models [2, 3]. We have widely investigated Lagrangian particle models evolving in a turbulent environment which is described from an Eulerian point of view. In this abstract we shortly review the methods employed: the models for particle dynamics together with the numerical m作者: 惰性女人 時(shí)間: 2025-3-26 08:11
Springer Monographs in Mathematicsses. We apply a pseudospectral method for the Cartesian case and a second-order finite difference method for the cylindrical one. The Prandtl number is . = 0.7 for all cases. The Rayleigh numbers . vary between 10. and 10.. Figure 1 shows a snapshot of the temperature field in the Cartesian cell. Cl作者: Indolent 時(shí)間: 2025-3-26 08:58
The Basics of Processes and Modelsresult, during the condensation stage the droplet population becomes more and more homogeneous, while the growth slows down. On the one hand, this slowing process cannot lead to a precipitation in reasonable times; on the other hand, the explosive process ensured by collisions cannot occur, if all t作者: 退潮 時(shí)間: 2025-3-26 16:08
Girjesh Govil,Ramakrishna V. Hosurhe bottom one is hot. The section of the cell is 40 × 10 cm. and its height is 40 cm. The thickness of the walls, made with PMMA, is 2 cm. Furthermore, two honeycomb structures allow to prevent convection from appearing in about 50% of the cell and, as we can see on Fig. 1, between these structures,作者: Forage飼料 時(shí)間: 2025-3-26 18:30 作者: 侵略者 時(shí)間: 2025-3-26 22:29
Pavel G. Khalatur,Alexei R. Khokhlov. For instance, existing numerical studies are limited within frameworks of a semi-realistic model [3] or of a tilted geometry with a minimal domain [4]. However, owing to the recent development of computers, DNS of the subcritical CF is now possible to be performed.作者: MERIT 時(shí)間: 2025-3-27 01:16
https://doi.org/10.1007/11570325an be used to predict directly from the fundamental equations physical quantities such as bulk flow rate and mean wall drag. All results and the code that generates them are disseminated through through our group‘s open-source CFD software and solution database Channelflow.org and the collaborative 作者: MUTED 時(shí)間: 2025-3-27 06:12 作者: heirloom 時(shí)間: 2025-3-27 09:28
Lagrangian analysis of turbulent convectionses. We apply a pseudospectral method for the Cartesian case and a second-order finite difference method for the cylindrical one. The Prandtl number is . = 0.7 for all cases. The Rayleigh numbers . vary between 10. and 10.. Figure 1 shows a snapshot of the temperature field in the Cartesian cell. Cl作者: Psa617 時(shí)間: 2025-3-27 17:30 作者: 晚來(lái)的提名 時(shí)間: 2025-3-27 19:31
Flow reversals in a vertical channelhe bottom one is hot. The section of the cell is 40 × 10 cm. and its height is 40 cm. The thickness of the walls, made with PMMA, is 2 cm. Furthermore, two honeycomb structures allow to prevent convection from appearing in about 50% of the cell and, as we can see on Fig. 1, between these structures,作者: 使閉塞 時(shí)間: 2025-3-27 22:01 作者: 褲子 時(shí)間: 2025-3-28 03:53
DNS of turbulent plane Couette flow with emphasis on turbulent stripe. For instance, existing numerical studies are limited within frameworks of a semi-realistic model [3] or of a tilted geometry with a minimal domain [4]. However, owing to the recent development of computers, DNS of the subcritical CF is now possible to be performed.作者: 上漲 時(shí)間: 2025-3-28 07:39 作者: 咯咯笑 時(shí)間: 2025-3-28 14:13 作者: 眉毛 時(shí)間: 2025-3-28 15:46 作者: CLAIM 時(shí)間: 2025-3-28 22:10
Conformance Checking and its Challengesdied particle dispersion in DNS of stationary strat-ified turbulence and observed a plateau with .. However, some of the DNS showed that . at long times caused by density changes of fluid particles by molecular diffusion.作者: hyperuricemia 時(shí)間: 2025-3-29 01:02 作者: Exclude 時(shí)間: 2025-3-29 04:09 作者: Ingest 時(shí)間: 2025-3-29 09:42
Conference proceedings 20091st editionts....MHD turbulence....Reacting and compressible turbulence....Transport and mixing....Turbulence in multiphase and non-Newtonian flows....?Vortex dynamics and structure formation....?Wall bounded flows..作者: 采納 時(shí)間: 2025-3-29 11:45
Parisa Hariri,Riku Klén,Matti Vuorinename physical properties at different Reynolds numbers and with different physical modeling. We discuss briefly the limitations of the point particle model and suggest a simple but effective way to extend it.作者: chastise 時(shí)間: 2025-3-29 18:34 作者: Inflamed 時(shí)間: 2025-3-29 23:00
The Basics of Processes and Modelscaying flows in a square and in a circular domain. The numerical set-up is described in [1, 4] and the Lagrangian statistics are averaged over 104 trajectories. The numerical resolution is . = 1024.. The initial eddy turn over time is . and the initial Reynolds number is ., where . is the initial kinetic energy and . is the size of the square.作者: 使混合 時(shí)間: 2025-3-30 01:34
Handling Noise and Incompletenessthis work is to employ coloured particles and use the associated separation into different colour classes. Considering separately each resulting colour class, the apparent particle density is decreased without restrictions in the measurement accuracy.作者: 健壯 時(shí)間: 2025-3-30 07:03
Amino Acids, Peptides and Proteins,e the three components of the velocity field in a meridian plane of the flow. Our acquisition frequency is moderate, around 10 Hz, but our system is able to record up to 32 000 velocity fields providing a large statistics and highly converged averages.作者: AVERT 時(shí)間: 2025-3-30 10:07
ary material: .This volume comprises the communications presented at the EUROMECH European .Turbulence Conference ETC12, held in Marburg in September 2009. The topics covered by the meeting include:.....Acoustics of turbulent flows????? ....Atmospheric turbulence....Control of turbulent flows....Geo作者: Ischemic-Stroke 時(shí)間: 2025-3-30 14:31 作者: flex336 時(shí)間: 2025-3-30 19:49 作者: Canvas 時(shí)間: 2025-3-30 21:46
Lagrangian modeling and properties of particles with inertiaame physical properties at different Reynolds numbers and with different physical modeling. We discuss briefly the limitations of the point particle model and suggest a simple but effective way to extend it.作者: 記憶 時(shí)間: 2025-3-31 03:36
Lagrangian statistics of inertial particles in turbulent flow then affected by so called inertial effects, deviates from that of fluid particles[1, 2, 3]. One critical and difficult point is to develop models which correctly describe the dynamics of particles over a wide range of sizes and density.作者: 排出 時(shí)間: 2025-3-31 07:01 作者: bile648 時(shí)間: 2025-3-31 10:41
3-D Particle Tracking Velocimetry (PTV) in gas flows using coloured tracer particlesthis work is to employ coloured particles and use the associated separation into different colour classes. Considering separately each resulting colour class, the apparent particle density is decreased without restrictions in the measurement accuracy.作者: Vo2-Max 時(shí)間: 2025-3-31 14:42
