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Journal articles on the topic 'Flow theory'

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Published: 4 June 2021
Last updated: 31 January 2023

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1

Cobb, J. A., and M. G. Gouda. "Flow theory." IEEE/ACM Transactions on Networking 5, no. 5 (1997): 661–74. http://dx.doi.org/10.1109/90.649567.

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2

CARDAO-PITO, TIAGO. "Intangible Flow Theory." American Journal of Economics and Sociology 71, no. 2 (April 2012): 328–53. http://dx.doi.org/10.1111/j.1536-7150.2012.00833.x.

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3

Ronen, R., A. D. Gat, M. Z. Bazant, and M. E. Suss. "Single-flow multiphase flow batteries: Theory." Electrochimica Acta 389 (September 2021): 138554. http://dx.doi.org/10.1016/j.electacta.2021.138554.

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4

Pak, Hong Kyung. "On Harmonic Theory in Flows." Canadian Mathematical Bulletin 46, no. 4 (December 1, 2003): 617–31. http://dx.doi.org/10.4153/cmb-2003-057-9.

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AbstractRecently [8], a harmonic theory was developed for a compact contact manifold from the viewpoint of the transversal geometry of contact flow. A contact flow is a typical example of geodesible flow. As a natural generalization of the contact flow, the present paper develops a harmonic theory for various flows on compact manifolds. We introduce the notions of H-harmonic and H*-harmonic spaces associated to a Hörmander flow. We also introduce the notions of basic harmonic spaces associated to a weak basic flow. One of our main results is to show that in the special case of isometric flow these harmonic spaces are isomorphic to the cohomology spaces of certain complexes. Moreover, we find an obstruction for a geodesible flow to be isometric.
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5

YANG, JIAGANG. "Cherry flow: physical measures and perturbation theory." Ergodic Theory and Dynamical Systems 37, no. 8 (May 12, 2016): 2671–88. http://dx.doi.org/10.1017/etds.2016.13.

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In this article we consider Cherry flows on the torus which have two singularities, a source and a saddle, and no periodic orbits. We show that every Cherry flow admits a unique physical measure, whose basin has full volume. This proves a conjecture given by Saghin and Vargas [Invariant measures for Cherry flows.Comm. Math. Phys.317(1) (2013), 55–67]. We also show that the perturbation of Cherry flows depends on the divergence at the saddle: when the divergence is negative, this flow admits a neighborhood, such that any flow in this neighborhood belongs to one of the following three cases: it has a saddle connection; it is a Cherry flow; it is a Morse–Smale flow whose non-wandering set consists of two singularities and one periodic sink. In contrast, when the divergence is non-negative, this flow can be approximated by a non-hyperbolic flow with an arbitrarily large number of periodic sinks.
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6

Gourdine, Christopher, Justin Edgren, Thomas Trice, and Joseph Zlatic. "Social Affinity Flow Theory." Journal of Bahá’í Studies 29, no. 4 (December 1, 2019): 53–80. http://dx.doi.org/10.31581/jbs-29.4.3(2019).

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This article presents a new theoretical construct, Social Affinity Flow Theory (SAFT), which both describes and predicts fl ow phenomena across a diversity of human social systems and is founded upon constructal law. Constructal law and its associated s-curves describe many phenomena, both in nature and in human societies. Extrapolated from the work of Bejan and Zane and integrating social science research, it provides a foundational explanation of social rifts prevalent in many societies today as well as constructive efforts of social change, whether secular or religiously based. A primary example of constructive change explained by SAFT is the community-building work of the Bahá’í Faith, as reflected in both its teachings and its training institute process.
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7

YAO, LUN-SHIN. "A resonant wave theory." Journal of Fluid Mechanics 395 (September 25, 1999): 237–51. http://dx.doi.org/10.1017/s0022112099005832.

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Analysis is used to show that a solution of the Navier–Stokes equations can be computed in terms of wave-like series, which are referred to as waves below. The mean flow is a wave of infinitely long wavelength and period; laminar flows contain only one wave, i.e. the mean flow. With a supercritical instability, there are a mean flow, a dominant wave and its harmonics. Under this scenario, the amplitude of the waves is determined by linear and nonlinear terms. The linear case is the target of flow-instability studies. The nonlinear case involves energy transfer among the waves satisfying resonance conditions so that the wavenumbers are discrete, form a denumerable set, and are homeomorphic to Cantor's set of rational numbers. Since an infinite number of these sets can exist over a finite real interval, nonlinear Navier–Stokes equations have multiple solutions and the initial conditions determine which particular set will be excited. Consequently, the influence of initial conditions can persist forever. This phenomenon has been observed for Couette–Taylor instability, turbulent mixing layers, wakes, jets, pipe flows, etc. This is a commonly known property of chaos.
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8

STONE, H. A. "Philip Saffman and viscous flow theory." Journal of Fluid Mechanics 409 (April 25, 2000): 165–83. http://dx.doi.org/10.1017/s0022112099007697.

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Philip Saffman made valuable theoretical contributions to different areas of low-Reynolds-number hydrodynamics. Three themes are selected for discussion here: (i) the lift force on a sphere in a shear flow at small, but finite Reynolds number, (ii) Brownian motion in thin liquid films, and (iii) particle motion in rapidly rotating flows. In addition, brief descriptions are given of some of Saffman's other contributions including dispersion in porous media, the average velocity of sedimenting suspensions, and compressible low-Reynolds-number flows.
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9

Daamen, Winnie, Serge P. Hoogendoorn, and Piet H. L. Bovy. "First-Order Pedestrian Traffic Flow Theory." Transportation Research Record: Journal of the Transportation Research Board 1934, no. 1 (January 2005): 43–52. http://dx.doi.org/10.1177/0361198105193400105.

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This paper discusses the validity of first-order traffic flow theory for the description of two-dimensional pedestrian flow operations in the case of an oversaturated bottleneck in front of which a large high-density region has formed. The paper shows how observations of density, speed, and flow that have been collected from laboratory walking experiments can be interpreted from the viewpoint of first-order theory. It is observed that pedestrians present at the same cross section inside of the congested region may encounter different flow conditions. This mainly depends on the lateral position of the pedestrian with respect to the center of the congested region. In the lateral center, high densities and low speeds are observed. However, on the boundary of the congested region, pedestrians may walk in nearly free-flow conditions and literally walk around this congested region. Visualization of these data in the flow– density plane results in a large scatter of points that have similar flows (bottleneck capacity) but different densities. This can be explained by noticing that observations of congestion of pedestrian traffic over the total width of the cross section do not belong to a single fundamental diagram but belong to a set of different fundamental diagrams. This observation has consequences for estimation of the fundamental diagram describing pedestrian traffic.
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10

Chernyshenko, S. I. "Asymptotic Theory of Global Separation." Applied Mechanics Reviews 51, no. 9 (September 1, 1998): 523–36. http://dx.doi.org/10.1115/1.3099021.

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This article aims to review the recent achievements and the state of the art in the high Reynolds number asymptotic theory of steady separated flow past bluff bodies for a general reader specializing in fluid dynamics who is not necessarily familiar with modern asymptotic techniques. A short historical overview is given. The ideas of the mathematical methods used are briefly outlined. Then the general structure of the solution for a plane flow past a bluff body is described. The physical mechanisms of such a flow are discussed, and quantitative results are given and compared with numerical calculations. Existing extensions of the theory and the latest results for axisymmetric flows are described. In conclusion, the relationship between asymptotic theory and real turbulent flows is discussed. This review article contains 76 references.
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11

COLEMAN, S. E., and J. D. FENTON. "Potential-flow instability theory and alluvial stream bed forms." Journal of Fluid Mechanics 418 (September 10, 2000): 101–17. http://dx.doi.org/10.1017/s0022112000001099.

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The present work constitutes a reassessment of the role of potential-flow analyses in describing alluvial-bed instability. To facilitate the analyses, a new potential-flow description of unsteady alluvial flow is presented, with arbitrary phase lags between local flow conditions and sediment transport permitted implicitly in the flow model. Based on the present model, the explicit phase lag between local sediment transport rate and local flow conditions adopted for previous potential-flow models is shown to be an artificial measure that results in model predictions that are not consistent with observed flow system behaviour. Previous potential-flow models thus do not provide correct descriptions of alluvial flows, and the understanding of bed-wave mechanics inferred based upon these models needs to be reassessed. In contrast to previous potential-flow models, the present one, without the use of an explicit phase lag, predicts instability of flow systems of rippled or dune-covered equilibrium beds. Instability is shown to occur at finite growth rates for a range of wavelengths via a resonance mechanism occurring for surface waves and bed waves travelling at the same celerity. In addition, bed-wave speeds are predicted to decrease with increasing wavelength, and bed waves are predicted to grow and move at faster rates for flows of larger Froude numbers. All predictions of the present potential-flow model are consistent with observations of physical flow systems. Based on the predicted unstable wavelengths for a given alluvial flow, it is concluded that bed waves are not generated from plane bed conditions by any potential-flow instability mechanism. The predictions of instability are nevertheless consistent with instances of accelerated wave growth occurring for flow systems of larger finite developing waves. Potential-flow description of alluvial flows should, however, no longer form the basis of instability analyses describing bed-form (sand-wavelet) generation from flat bed conditions.
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12

Chung, Kwansoo, and Sergei Alexandrov. "Ideal Flow in Plasticity." Applied Mechanics Reviews 60, no. 6 (November 1, 2007): 316–35. http://dx.doi.org/10.1115/1.2804331.

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Ideal plastic flows constitute a class of solutions in the classical theory of plasticity based on, especially for bulk forming cases, Tresca’s yield criterion without hardening and its associated flow rule. They are defined by the condition that all material elements follow the minimum plastic work path, a condition which is believed to be advantageous for forming processes. Thus, the ideal flow theory has been proposed as the basis of procedures for the direct preliminary design of forming processes, which mainly involve plastic deformation. The aim of the present review is to provide a summary of both the theory of ideal flows and its applications. The theory includes steady and nonsteady flows, which are divided into three sections, respectively: plane-strain flows, axisymmetric flows, and three-dimensional flows. The role of the method of characteristics, including the computational aspect, is emphasized. The theory of ideal membrane flows is also included but separately because of its advanced applications based on finite element numerical codes. For membrane flows, restrictions on the constitutive behavior of materials are significantly relaxed so that more sophisticated anisotropic constitutive laws with hardening are accounted for. In applications, the ideal plastic flow theory provides not only process design guidelines for current forming processes under realistic tool constraints, but also proposes new ultimate optimum process information for futuristic processes.
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13

Ahamed, Syed, and Sonya Ahamed. "Conductive Flow Theory of Knowledge." British Journal of Applied Science & Technology 10, no. 3 (January 10, 2015): 1–17. http://dx.doi.org/10.9734/bjast/2015/14740.

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14

Chi, R. M. "Separated flow unsteady aerodynamic theory." Journal of Aircraft 22, no. 11 (November 1985): 956–64. http://dx.doi.org/10.2514/3.45231.

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15

Ottinger, P. F., and J. W. Schumer. "Magnetically insulated ion flow theory." Physics of Plasmas 13, no. 6 (June 2006): 063101. http://dx.doi.org/10.1063/1.2207122.

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16

Zhou, Xin-Wei. "Variational theory for physiological flow." Computers & Mathematics with Applications 54, no. 7-8 (October 2007): 1000–1002. http://dx.doi.org/10.1016/j.camwa.2006.12.043.

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17

Sopasakis, A. "Unstable flow theory and modeling,." Mathematical and Computer Modelling 35, no. 5-6 (March 2002): 623–41. http://dx.doi.org/10.1016/s0895-7177(01)00186-8.

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18

Sopasakis, A. "Unstable flow theory and modeling." Mathematical and Computer Modelling 35, no. 5-6 (March 2002): 623–41. http://dx.doi.org/10.1016/s0895-7177(02)80025-5.

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19

Bergholm, Fredrik, and Stefan Carlsson. "A “theory” of optical flow." CVGIP: Image Understanding 53, no. 2 (March 1991): 171–88. http://dx.doi.org/10.1016/1049-9660(91)90025-k.

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20

Zhi, Gao. "Viscous-inviscid interacting flow theory." Acta Mechanica Sinica 6, no. 2 (May 1990): 102–10. http://dx.doi.org/10.1007/bf02488440.

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21

Streets, Jeffrey, and Gang Tian. "Regularity theory for pluriclosed flow." Comptes Rendus Mathematique 349, no. 1-2 (January 2011): 1–4. http://dx.doi.org/10.1016/j.crma.2010.11.014.

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22

Piest, Jürgen. "Theory of turbulent shear flow." Physica A: Statistical Mechanics and its Applications 157, no. 2 (June 1989): 688–704. http://dx.doi.org/10.1016/0378-4371(89)90062-9.

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23

Piest, Jürgen. "Theory of turbulent shear flow." Physica A: Statistical Mechanics and its Applications 168, no. 3 (October 1990): 966–82. http://dx.doi.org/10.1016/0378-4371(90)90266-u.

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24

Piest, Jürgen. "Theory of turbulent shear flow." Physica A: Statistical Mechanics and its Applications 187, no. 1-2 (August 1992): 172–90. http://dx.doi.org/10.1016/0378-4371(92)90417-o.

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25

Janner, Rémi, and Jan Swoboda. "Elliptic Yang-Mills flow theory." Mathematische Nachrichten 288, no. 8-9 (February 18, 2015): 935–67. http://dx.doi.org/10.1002/mana.201400109.

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26

Serra, Mattia, Jérôme Vétel, and George Haller. "Exact theory of material spike formation in flow separation." Journal of Fluid Mechanics 845 (April 20, 2018): 51–92. http://dx.doi.org/10.1017/jfm.2018.206.

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We develop a frame-invariant theory of material spike formation during flow separation over a no-slip boundary in two-dimensional flows with arbitrary time dependence. Based on the exact curvature evolution of near-wall material lines, our theory identifies both fixed and moving flow separation, is effective also over short time intervals, and admits a rigorous instantaneous limit. As a byproduct, we derive explicit formulae for the evolution of material line curvature and the curvature rate for general compressible flows. The material backbone that we identify acts first as the precursor and later as the centrepiece of unsteady Lagrangian flow separation. We also discover a previously undetected spiking point where the backbone of separation connects to the boundary, and derive wall-based analytical formulae for its location. Finally, our theory explains the perception of off-wall separation in unsteady flows and provides conditions under which such a perception is justified. We illustrate our results on several analytical and experimental flows.
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27

Silberschatz, Marc. "Creative State / Flow State: Flow Theory in Stanislavsky's Practice." New Theatre Quarterly 29, no. 1 (February 2013): 13–23. http://dx.doi.org/10.1017/s0266464x1300002x.

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Nearly seventy-five years after his death, Konstantin Stanislavsky remains a toweringly influential figure, and many fundamental ideas about acting can be traced back to his practice. In this article, Marc Silberschatz examines the correspondences with, and divergences from, flow theory – the theory surrounding the psychological state associated with ‘being in the zone’ – in Stanislavsky's practice. Although separated by vast differences in social, cultural, and historical context, some significant and increasing correspondences between flow theory and Stanislavsky's practice are revealed and examined. Additionally, divergences from flow theory are identified and interrogated, suggesting that Stanislavsky's reliance on fixed, repeatable performance scores and divided consciousness are direct impediments to the achievement of flow. Marc Silberschatz is a PhD candidate at the Royal Conservatoire of Scotland. He is also a professional theatre director whose work has been seen in both the United States and Scotland.
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28

Schmid-Scho¨nbein, G. W. "A Theory of Blood Flow in Skeletal Muscle." Journal of Biomechanical Engineering 110, no. 1 (February 1, 1988): 20–26. http://dx.doi.org/10.1115/1.3108401.

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A theoretical analysis of blood flow in the microcirculation of skeletal muscle is provided. The flow in the microvessels of this organ is quasi steady and has a very low Reynolds number. The blood is non-Newtonian and the blood vessels are distensible with viscoelastic properties. A formulation of the problem is provided using a viscoelastic model for the vessel wall which was recently derived from measurements in the rat spinotrapezius muscle (Skalak and Schmid-Scho¨nbein, 1986b). Closed form solutions are derived for several physiologically important cases, such as perfusion at steady state, transient and oscillatory flows. The results show that resting skeletal muscle has, over a wide range of perfusion pressures an almost linear pressure-flow curve. At low flow it exhibits nonlinearities. Vessel distensibility and the non-Newtonian properties of blood both have a strong influence on the shape of the pressure-flow curve. During oscillatory flow the muscle exhibits hysteresis. The theoretical results are in qualitative agreement with experimental observations.
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29

Bagheri, S., and D. S. Henningson. "Transition delay using control theory." Philosophical Transactions of the Royal Society A: Mathematical, Physical and Engineering Sciences 369, no. 1940 (April 13, 2011): 1365–81. http://dx.doi.org/10.1098/rsta.2010.0358.

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This review gives an account of recent research efforts to use feedback control for the delay of laminar–turbulent transition in wall-bounded shear flows. The emphasis is on reducing the growth of small-amplitude disturbances in the boundary layer using numerical simulations and a linear control approach. Starting with the application of classical control theory to two-dimensional perturbations developing in spatially invariant flows, flow control based on control theory has progressed towards more realistic three-dimensional, spatially inhomogeneous flow configurations with localized sensing/actuation. The development of low-dimensional models of the Navier–Stokes equations has played a key role in this progress. Moreover, shortcomings and future challenges, as well as recent experimental advances in this multi-disciplinary field, are discussed.
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30

Paidoussis, M. P., S. J. Price, and D. Mavriplis. "A Semipotential Flow Theory for the Dynamics of Cylinder Arrays in Cross Flow." Journal of Fluids Engineering 107, no. 4 (December 1, 1985): 500–506. http://dx.doi.org/10.1115/1.3242520.

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This paper presents a semianalytical model, involving the superposition of the empirically determined cross flow about a cylinder in an array and the analytically determined vibration-induced flow field in still fluid, for the purpose of analyzing the stability of cylinder arrays in cross flow and predicting the threshold of fluidelastic instability. The flow field is divided into two regions: a viscous bubble of separated flow, and an inviscid, sinuous duct-flow region elsewhere. The only empirical input required by the model in its simplest form is the pressure distribution about a cylinder in the array. The results obtained are in reasonably good accord with experimental data, only for low values of the mass-damping parameter (e.g., for liquid flows), where fluidelastic instability is predominantly caused by negative fluid-dynamic damping terms. For high mass-damping parameters (e.g., for gaseous flows), where fluidelastic instability is evidently controlled by fluid-dynamic stiffness terms, the model greatly overestimates the threshold of fluidelastic instability. However, once measured fluid-dynamic stiffness terms are included in the model, agreement with experimental data is much improved, yielding the threshold flow velocities for fluidelastic instability to within a factor of 2 or better.
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31

Matoušek, Václav, and Štěpán Zrostlík. "Bed Load Transport Modelling Using Kinetic Theory." E3S Web of Conferences 40 (2018): 05072. http://dx.doi.org/10.1051/e3sconf/20184005072.

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Intense transport of bed load is associated with highconcentrated sediment-laden flow over a plane mobile bed at high bed shear. Typically, the flow exhibits a layered internal structure in which a vast majority of sediment grains is transported through a collisional layer above the bed. Our investigation focuses on steady uniform open-channel flow with a developed collisional transport layer and combines modelling and experiment to relate integral quantities, as the discharge of solids, discharge of mixture, and flow depth with the longitudinal slope of the bed and the internal structure of the flow above the bed. In the paper, flow with the internal structure described by linear vertical distributions of granular velocity and concentration across the collisional layer is analyzed by a model based on the classical kinetic theory of granular flows. The model predicts the total discharge, the discharge of sediment, and the flow depth for given (experimentally determined) bed slope and thickness of collisional layer. The model also predicts whether the intefacial dense layer develops between the bed and the collisional layer and how thick it is. Model predictions are compared with results of intense bed-load experiment carried out for lightweight sediment in our laboratory tilting flume.
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32

Kurz, Heinz D., and Neri Salvadori. "Fund–flow versus flow–flow in production theory: Reflections on Georgescu-Roegen’s contribution." Journal of Economic Behavior & Organization 51, no. 4 (August 2003): 487–505. http://dx.doi.org/10.1016/s0167-2681(02)00143-9.

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33

Bent, J. "Neutron-Mapping Polymer Flow: Scattering, Flow Visualization, and Molecular Theory." Science 301, no. 5640 (September 19, 2003): 1691–95. http://dx.doi.org/10.1126/science.1086952.

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34

Zhang, Yonghao, David R. Emerson, and Jason M. Reese. "General theory for flow optimisation of split-flow thin fractionation." Journal of Chromatography A 1010, no. 1 (August 2003): 87–94. http://dx.doi.org/10.1016/s0021-9673(03)01025-2.

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35

Teng, Ching-I., and Han-Chung Huang. "More Than Flow: Revisiting the Theory of Four Channels of Flow." International Journal of Computer Games Technology 2012 (2012): 1–9. http://dx.doi.org/10.1155/2012/724917.

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Flow (FCF) theory has received considerable attention in recent decades. In addition to flow, FCF theory proposed three influential factors, that is, boredom, frustration, and apathy. While these factors have received relatively less attention than flow, Internet applications have grown exponentially, warranting a closer reexamination of the applicability of the FCF theory. Thus, this study tested the theory that high/low levels of skill and challenge lead to four channels of flow. The study sample included 253 online gamers who provided valid responses to an online survey. Analytical results support the FCF theory, although a few exceptions were noted. First, skill was insignificantly related to apathy, possibly because low-skill users can realize significant achievements to compensate for their apathy. Moreover, in contrast with the FCF theory, challenge was positively related to boredom, revealing that gamers become bored with difficult yet repetitive challenges. Two important findings suggest new directions for FCF theory.
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36

Page, R. H., L. L. Hadden, and C. Ostowari. "Theory for Radial Jet Reattachment Flow." AIAA Journal 28, no. 7 (July 1990): 1338b. http://dx.doi.org/10.2514/3.48892.

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37

Tong, Bing-Gang, and W. H. Hui. "Unsteady embedded Newton-Busemann flow theory." Journal of Spacecraft and Rockets 23, no. 2 (March 1986): 129–35. http://dx.doi.org/10.2514/3.25798.

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38

Kerner, Boris S. "Congested Traffic Flow: Observations and Theory." Transportation Research Record: Journal of the Transportation Research Board 1678, no. 1 (January 1999): 160–67. http://dx.doi.org/10.3141/1678-20.

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39

Page, R. H., L. L. Hadden, and C. Ostowari. "Theory for radial jet reattachment flow." AIAA Journal 27, no. 11 (November 1989): 1500–1505. http://dx.doi.org/10.2514/3.10294.

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40

Poorooshasb, H. B., and S. Pietruszczak. "A Generalized Flow Theory for Sand." Soils and Foundations 26, no. 2 (June 1986): 1–15. http://dx.doi.org/10.3208/sandf1972.26.2_1.

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41

Gray, William G., and S. Majid Hassanizadeh. "Unsaturated Flow Theory Including Interfacial Phenomena." Water Resources Research 27, no. 8 (August 1991): 1855–63. http://dx.doi.org/10.1029/91wr01260.

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42

Singh, Vijay P., Aaron Byrd, and Huijuan Cui. "Flow Duration Curve Using Entropy Theory." Journal of Hydrologic Engineering 19, no. 7 (July 2014): 1340–48. http://dx.doi.org/10.1061/(asce)he.1943-5584.0000930.

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43

Kleinstreuer,, C., and P. Griffith,. "Two-Phase Flow: Theory and Applications." Applied Mechanics Reviews 57, no. 4 (July 1, 2004): B22—B23. http://dx.doi.org/10.1115/1.1786590.

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44

Zhang, H. M. "A theory of nonequilibrium traffic flow." Transportation Research Part B: Methodological 32, no. 7 (September 1998): 485–98. http://dx.doi.org/10.1016/s0191-2615(98)00014-9.

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45

Aguilera, N�stor E. "Numerical analysis of cavitational flow-theory." Numerische Mathematik 55, no. 1 (January 1989): 1–32. http://dx.doi.org/10.1007/bf01395870.

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46

Wang, Junye. "Theory of flow distribution in manifolds." Chemical Engineering Journal 168, no. 3 (April 2011): 1331–45. http://dx.doi.org/10.1016/j.cej.2011.02.050.

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47

Wichman, Indrek S. "Theory of opposed-flow flame spread." Progress in Energy and Combustion Science 18, no. 6 (January 1992): 553–93. http://dx.doi.org/10.1016/0360-1285(92)90039-4.

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48

Li, Yongsheng, and Yoshio Narusawa. "Zone circulating flow-injection analysis: theory." Analytica Chimica Acta 289, no. 3 (May 1994): 355–64. http://dx.doi.org/10.1016/0003-2670(94)90012-y.

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49

Song, Bohui, and Shoubo Xu. "The theory of material flow substance." Systems Research and Behavioral Science 26, no. 2 (March 2009): 251–58. http://dx.doi.org/10.1002/sres.969.

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50

Smul’skii, I. I. "A sink-flow theory of tornados." Journal of Engineering Physics and Thermophysics 70, no. 6 (November 1997): 941–51. http://dx.doi.org/10.1007/s10891-997-0046-4.

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Dissertations / Theses Books
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