Article records
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A Caltech Library Repository Feedhttp://www.rssboard.org/rss-specificationpython-feedgenenFri, 08 Dec 2023 12:22:48 +0000A two-dimensional sink in a density-stratified porous medium
https://resolver.caltech.edu/CaltechAUTHORS:20160418-124108630
Authors: List, E. J.
Year: 1968
DOI: 10.1017/S0022112068001497
A solution is offered for the flow induced by a two-dimensional line sink in a saturated, density-stratified porous medium. It is found that fluid is selectively withdrawn from a thin layer at the elevation of the line sink and not from the entire medium. The velocity distributions predicted by the theory are checked by experiments in a Hele–Shaw cell and good agreement found.https://authors.library.caltech.edu/records/wxn6a-9ry95An exact solution for a diffusive flow in a porous medium
https://resolver.caltech.edu/CaltechAUTHORS:20160418-124620937
Authors: List, E. J.
Year: 1969
DOI: 10.1017/S0022112069001479
It is shown that Yih's exact solution for the non-diffusive flow of a non-homogeneous fluid into a sink in a confined porous medium is equivalent to a class of diffusive flows with isopycnic lateral boundaries.https://authors.library.caltech.edu/records/rb24a-ez081Laminar momentum jets in a stratified fluid
https://resolver.caltech.edu/CaltechAUTHORS:20160418-123344546
Authors: List, E. J.
Year: 1971
DOI: 10.1017/S0022112071000193
Solutions are presented for creeping flows induced by two-and three-dimensional horizontal and vertical momentum jets in a linearly stratified unbounded diffusive viscous fluid. These linear problems are solved by replacing the momentum jet by a body force singularity represented by delta functions and solving the partial differential equations of motion by use of multi-dimensional Fourier transforms. The integral representations for the physical variables are evaluated by a combination of residue theory and numerical integration.
The solutions for vertical jets show the jet to be trapped within a layer of finite thickness and systems of rotors to be induced. The horizontal two-dimensional jet solution shows return flows above and below the jet and a pair of rotors. The three-dimensional horizontal jet has no return flow at finite distance and the diffusive contribution is found to be almost negligible in most situations, the primary character of the horizontal flows being given by the non-diffusive solution. Stokes's paradox is found to be non-existent in a density-stratified fluid.https://authors.library.caltech.edu/records/2aerr-p4a24Variations in coastal temperatures on the southern and central California coast
https://resolver.caltech.edu/CaltechAUTHORS:20170419-084049797
Authors: List, E. J.; Koh, R. C. Y.
Year: 1976
DOI: 10.1029/JC081i012p01971
The results of a time series analysis of several years of coastal ocean temperature records are presented for discussion. The records have been analyzed by using digital filtering, covariance and spectral analysis. The low-frequency component of the temperature signal shows a strong seasonal component in southern California. There is little seasonal fluctuation between Point Conception and Pacific Grove. A period of midwinter warming is apparent in southern California. Intermediate frequency components show strong correlations in southern California with the presence of distinct and substantial temperature events occurring almost simultaneously over distances of the order of 200 km. High-frequency components have a large standard deviation in summer (0.8°C) and a low standard deviation in winter (0.4°C); these components are uncorrelated at stations even a few miles apart. Some coastal stations show a strong possible diurnal component; others, including the offshore islands, show no such components. Morro Bay appears to have an extraordinarily large diurnal component of temperature fluctuation. No attempt has been made in this paper to relate these phenomena to other oceanographic or meteorological variables.https://authors.library.caltech.edu/records/hyrmz-bsf61Plane turbulent buoyant jets. Part 1. Integral properties
https://resolver.caltech.edu/CaltechAUTHORS:KOTjfm77a
Authors: Kotsovinos, Nikolas E.; List, E. John
Year: 1977
DOI: 10.1017/S002211207700189X
An integral technique suggested for the analysis of turbulent jets by Corrsin & Uberoi (1950) and Morton, Taylor & Turner (1956) is re-examined in an attempt to improve the description of the entrainment. It is determined that the hypothesis of Priestley & Ball (1955), that the entrainment coefficient is a linear function of the jet Richardson number, is reasonable, and that two empirically determined plume parameters are sufficient to describe the transition of buoyant jets to plumes. The results of a series of experiments in which both time-averaged velocity and time-averaged temperature profiles were recorded in a substantial number of plane turbulent buoyant jets of varying initial Richardson numbers are used to verify the basic ideas. In addition, measurements of the mean tracer flux in a series of buoyant jets indicate that as much as 40% of the transport in plumes is by the turbulent flux.https://authors.library.caltech.edu/records/dc9yy-ffy05Turbulent Jets and Plumes
https://resolver.caltech.edu/CaltechAUTHORS:20161019-133155006
Authors: List, E. J.
Year: 1982
DOI: 10.1146/annurev.fl.14.010182.001201
Turbulent jets are fluid flows produced by a pressure drop through an orifice. Their mechanics, although studied for over fifty years, has recently received research attention that has resulted in a much improved understanding of the process by which they entrain surrounding fluid. Turbulent plumes are fluid motions whose primary source of kinetic energy and momentum flux is body forces derived from density inhomogeneities. Plumes have not been studied in the same detail as jets but nevertheless there have been some recent gains in the understanding of their mechanics. In this article we will review this progress, especially in relation to how jets and plumes interact with environmental factors, such as density stratification or uniform motion of the ambient fluid. As will become evident, many problems remain and, in some circumstances, we simply cannot describe precisely what does occur. In such cases we will try to provide current references and suggest approaches for future research.https://authors.library.caltech.edu/records/esa8f-pf112Collision efficiencies of diffusing spherical particles: hydrodynamic, van der Waals and electrostatic forces
https://resolver.caltech.edu/CaltechAUTHORS:20140922-104615615
Authors: Valioulis, Iraklis A.; List, E. John
Year: 1984
DOI: 10.1016/0001-8686(84)80001-9
A practical limitation of the application of Smoluchowski's classical estimate for the collisions probability of two diffusing spherical particles in Brownian motion is the non-consideration of interparticle forcves. For suspended particles in water such forces can arise from the disturbance the particle causes in the fluid (hydrodynamic forces), from the cloud of ions which surround an electrically charged particle (double layer forces) or they can be of molecular origin (van der Waals forces). In this paper corrections to Smoluckhowski's collision probability are computed when such forces operate Scoluchowski's collision probability are computed when such forces operate between two approaching particles of various sizes. Results for several values of the van der Waals energy of attraction and the ionic strength of the electrolyte are presented in a way convenient for particle collision modeling.https://authors.library.caltech.edu/records/ezyye-4q560Numerical simulation of a sedimentation basin. 2. Design application
https://resolver.caltech.edu/CaltechAUTHORS:20140917-101040541
Authors: Valioulis, Iraklis A.; List, E. John
Year: 1984
DOI: 10.1021/es00122a007
A numerical model of a rectangular settling tank is used
to study the importance of selective variables on the settling process while demonstrating the capabilities of the
computer simulation. The computer model follows the spatial and temporal development of the influent particle size distribution toward the outlet of the tank based on
the fundamental mechanisms which govern particle motion
and growth. It is shown that both the removal efficiency
of a flocculating suspension and the effluent particle size
distribution are influenced strongly by the mass concentration in the inflow, the influent particle size distribution, the floc size-density relationship, and the collision efficiencies of the particles. It is suggested that future experimental work should focus on obtaining information on the size-density relationship, the reentrainment of the deposits, and the collision efficiencies of floes.https://authors.library.caltech.edu/records/tcrq6-88h35Numerical Simulation of a Sedimentation Basin. 1. Model Development
https://resolver.caltech.edu/CaltechAUTHORS:20140922-103532038
Authors: Valioulis, Iraklis A.; List, E. John
Year: 1984
DOI: 10.1021/es00122a006
A method for the numerical simulation of a rectangular
sedimentation basin operating under steady or unsteady
conditions is described. The computer model follows the
spatial and temporal development of the influent particle
size distribution toward the outlet of the tank. It is based
on the fundamental mechanisms which govern particle
motion and growth. The model accounts for the variability
of the flow field and the particle size distribution in the
tank and, from the local development of the particle size
spectrum, predicts the overall performance of the settling
basin.https://authors.library.caltech.edu/records/6pkeb-a7s87Monte Carlo simulation of coagulation in discrete particle-size distributions. Part 2. Interparticle forces and the quasi-stationary equilibrium hypothesis
https://resolver.caltech.edu/CaltechAUTHORS:20120709-080438815
Authors: Valioulis, I. A.; List, E. J.; Pearson, H. J.
Year: 1984
DOI: 10.1017/S0022112084001403
Hunt (1982) and Friedlander (1960a, b) used dimensional analysis to derive expressions for the steady-state particle-size distribution in aerosols and hydrosols. Their results were supported by the Monte Carlo simulation of a non-interacting coagulating population of suspended spherical particles developed by Pearson, Valioulis & List (1984). Here the realism of the Monte Carlo simulation is improved by accounting for the modification to the coagulation rate caused by van der Waals', electrostatic and hydrodynamic forces acting between particles. The results indicate that the major hypothesis underlying the dimensional reasoning, that is, collisions between particles of similar size are most important in determining the shape of the particle size distribution, is valid only for shear-induced coagulation. It is shown that dimensional analysis cannot, in general, be used to predict equilibrium particle-size distributions, mainly because of the strong dependence of the interparticle force on the absolute and relative size of the interacting particles.https://authors.library.caltech.edu/records/ygfm5-50a22Monte Carlo simulation of coagulation in discrete particle-size distributions. Part 1. Brownian motion and fluid shearing
https://resolver.caltech.edu/CaltechAUTHORS:20120709-072813258
Authors: Pearson, H. J.; Valioulis, I. A.; List, E. J.
Year: 1984
DOI: 10.1017/S0022112084001397
A method for the Monte Carlo simulation, by digital computer, of the evolution of a colliding and coagulating population of suspended particles is described. Collision mechanisms studied both separately and in combination are: Brownian motion of the particles, and laminar and isotropic turbulent shearing motions of the suspending fluid. Steady-state distributions are obtained by adding unit-size particles at a constant rate and removing all particles once they reach a preset maximum volume. The resulting size distributions are found to agree with those obtained by dimensional analysis (Hunt 1982).https://authors.library.caltech.edu/records/x8y4d-6bg64A Numerical Evaluation of the Stochastic Completeness of the Kinetic Coagulation Equation
https://resolver.caltech.edu/CaltechAUTHORS:VALjas84
Authors: Valioulis, Iraklis A.; List, E. John
Year: 1984
DOI: 10.1175/1520-0469(1984)041<2516:ANEOTS>2.0.CO;2
The stochastic completeness of the kinetic coagulation equation depends on the extent of correlations between particle properties. Such correlations are induced by the coalescence process that causes spatial inhomogeneities in the number concentration of the particles, and are particularly strong in poorly mixed suspensions. A Monte Carlo simulation of the coalescence process is used to evaluate the suitability of the kinetic coagulation equation to simulate the coalescence process using Brownian diffusion, fluid shear and differential sedimentation collision kernels. It is demonstrated that the outcome of the kinetic equation matches well the true stochastic averages, unless the number concentration of particles involved is very small. In that case, the discrepancies between the two approaches are substantial in the large end of the particle size spectrum.https://authors.library.caltech.edu/records/n8xsk-nma53Turbulent mixing at a shear-free density interface
https://resolver.caltech.edu/CaltechAUTHORS:20160418-133752149
Authors: Hannoun, Imad A.; List, E. John
Year: 1988
DOI: 10.1017/S0022112088000977
The interaction of a sharp density interface with oscillating-grid-induced shear-free turbulence was experimentally investigated. A linear photodiode array was used in conjunction with laser-induced fluorescence to measure the concentration of dye that was initially only in the less dense layer. A laser-Doppler velocimeter was used to measure the vertical velocity in and above the density interface at a point where the dye concentration was also measured. Potential refractive-index-fluctuation problems were avoided using solutes that provided a homogeneous optical environment across the density interface. Internal wave spectra, amplitudes and velocities, as well as the vertical mass flux were measured. The results indicate that mixing occurs in intermittent bursts and that the gradient (local) Richardson number remains constant for a certain range of the overall Richardson number R_j, defined in terms of an integral lengthscale, buoyancy jump and turbulence intensity. The spectra of the internal waves decay as f^(−3) at frequencies below the maximum Brunt-Väisälä frequency. These findings give support to a model for oceanic mixing proposed by Phillips (1977) in which the internal waves are limited in their spectral density by sporadic local instabilities and breakdown to turbulence. The results also indicate that, for a certain R_j range, the thickness of the interfacial layer (normalized by the integral lengthscale of the turbulence) is a decreasing function of R_j. At sufficiently high R_j the interfacial thickness becomes limited by diffusive effects. Finally, we discuss a simple model for entrainment at a density interface in the presence of shear-free turbulence.https://authors.library.caltech.edu/records/6cxvn-wjc32Turbulence structure near a sharp density interface
https://resolver.caltech.edu/CaltechAUTHORS:20160418-151749264
Authors: Hannoun, Imad A.; Fernando, Harindra J. S.; List, E. John
Year: 1988
DOI: 10.1017/S0022112088000965
The effects of a sharp density interface and a rigid flat plate on oscillating-grid induced shear-free turbulence were investigated experimentally. A two-component laser-Doppler velocimeter was used to measure turbulence intensities in and above the density interface (with matched refractive indices) and near the rigid flat plate. Energy spectra, velocity correlations, and kinetic energy fluxes were also measured. Amplification of the horizontal turbulent velocity, coupled with a sharp reduction in the vertical turbulent velocity, was observed near both the density interface and the flat plate. These findings are in agreement with some previous results pertaining to shear-free turbulence near rigid walls (Hunt & Graham 1978) and near density interfaces (Long 1978). The results imply that, near the density interface, the turbulent kinetic energy in the vertical velocity component is only a small fraction of the total turbulent kinetic energy and indicate that the effects of the anisotropy created by the density interface or the flat plate are confined to the large turbulence scales.https://authors.library.caltech.edu/records/0da7v-h8z80Investigations of round vertical turbulent buoyant jets
https://resolver.caltech.edu/CaltechAUTHORS:20160418-152319876
Authors: Papanicolaou, Panos N.; List, E. John
Year: 1988
DOI: 10.1017/S0022112088002447
The axial and radial velocity components w and u, and the concentration c of a Rhodamine 6G dye were measured simultaneously in a turbulent buoyant jet, using laser-Doppler anemometry combined with a recently developed laser-induced-fluorescence concentration measurement technique. These non-intrusive techniques enable measurements in a region of plume motion where conventional probe-based techniques have had difficulties. The results of the study show that the asymptotic decay laws for velocity and concentration of a tracer transported by the flow are verified experimentally in both jets and plumes. The momentum and volume fluxes and the mean dilution factor are determined in dimensionless form as a function of the normalized distance from the flow source. Contradictory results from earlier experimental plume investigations concerning the decay laws of w and c and the plume width ratio b_c/b_w are discussed. The turbulence properties and the transition from momentum-driven jets to buoyancy-driven plumes are presented. The turbulence is found to scale with the mean flow as predicted by dimensional analysis and self-similarity. Buoyancy-produced turbulence is found to transport twice as much tracer as jet turbulence. Although velocity statistics in jets and plumes are found to be highly self-similar there is a strong disparity in the distribution of tracer concentration in the two flows. This occurs in the time-average mean flows as well as the r.m.s. turbulent quantities. Instantaneous concentration fluctuations are found to exceed time averages by as much as a factor of 3. The experimental results should provide a reasonable basis for validation of computer models of axisymmetric plumes.https://authors.library.caltech.edu/records/k4bya-erm31Large-scale structure in the far field of buoyant jets
https://resolver.caltech.edu/CaltechAUTHORS:20160418-152805105
Authors: Papantoniou, Dimitris; List, E. John
Year: 1989
DOI: 10.1017/S002211208900306X
The flow structure and entrainment mechanisms in the far field of a round vertical buoyant jet have been studied experimentally by use of an optical technique based on laser-induced fluorescence (LIF). A large number of essentially instantaneous tracer concentration profiles were recorded for each experimental run by combining LIF with linear photodiode array imaging and high-speed digital data acquisition. Analysis of the resulting high-resolution flow images indicates that the far-field region is dominated by the periodic passage of structures spanning the entire radial flow extent. Ambient fluid is entrained by vortical motions and is transported to regions deep into the flow interior. Correlation analysis discloses that the passage frequency of the structures scales with the local mean velocity and flow width. Conditional averaging of the data indicates that the downstream frontal region of the structure is well mixed and at higher concentration level than the back and side regions where ambient fluid is intermittently present. This results in an axial concentration gradient within the structure, analogous to the ramp-like pattern previously observed in heated air jets. In comparison to the momentum-driven flow the ambient fluid presence in the flow interior is greatly increased when body forces are the driving mechanism. This appears to result from the influence of buoyancy forces in the production of turbulent vortices at the integral scale. An important feature of both the momentum-driven and buoyancy-driven flows investigated is the strongly intermittent character of the concentration field. This raises the issue of the appropriateness of gradient-diffusion theories for the description of such flows.https://authors.library.caltech.edu/records/q84vj-b2k96On mixing and transport at a sheared density interface
https://resolver.caltech.edu/CaltechAUTHORS:20160418-125123356
Authors: Sullivan, Greg D.; List, E. John
Year: 1994
DOI: 10.1017/S0022112094001916
Mixing and transport of a stratifying scalar are investigated at a density interface imbedded in a turbulent shear flow. Steady-state interfacial shear flows are generated in a laboratory water channel for layer Richardson numbers, Ri, between about 1 and 10. The flow field is made optically homogeneous, enabling the use of laser-induced fluorescence with photodiode array imaging to measure the concentration field at high resolution. False-colour images of the concentration field provide valuable insight into interfacial dynamics: when the local mean shear Richardson number, Ri_s, is less than about 0.40–0.45, interfacial mixing appears to be dominated by Kelvin–Helmholtz (K–H) instabilities; when Ri_s is somewhat larger than this, interfacial mixing appears to be dominated by shear-driven wave breaking. In both cases, vertical transport of mixed fluid from the interfacial region into adjacent turbulent layers is accomplished by large-scale turbulent eddies which impinge on the interface and scour fluid from its outer edges.
Motivated by the experimental findings, a model for interfacial mixing and entrainment is developed. A local equilibrium is assumed in which the rate of loss of interfacial fluid by eddy scouring is balanced by the rate of production (local mixing) by interfacial instabilities and molecular diffusion. When a single layer is turbulent and entraining, the model results are as follows: in the molecular-diffusion-dominated regime, δ/h ~ Pe^(−1/2) and E ~ Ri^(−1)Pe^(−1/2); in the wave-breaking-dominated regime, δ/h ~ Ri^(−1/2) and E ~ Ri^(−3/2); and in the K–H-dominated regime, δ/h ~ Ri^(−1) and E ~ Ri^(−2), where δ is the interface thickness, h is the boundary-layer thickness, Pe is the Péclet number, and E is the normalized entrainment velocity. In all three regimes, the maximum concentration anomaly, Γ_m ~ Ri^(−1). When both layers are turbulent and entraining, E and δ depend on combinations of parameters from both layers.https://authors.library.caltech.edu/records/h1r96-xdy68