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Journal articles on the topic 'Fluid behavior'

Author: Grafiati

Published: 4 June 2021

Last updated: 9 February 2022

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1

Yasappan, Justine, Ángela Jiménez-Casas, and Mario Castro. "Asymptotic Behavior of a Viscoelastic Fluid in a Closed Loop Thermosyphon: Physical Derivation, Asymptotic Analysis, and Numerical Experiments." Abstract and Applied Analysis 2013 (2013): 1–20. http://dx.doi.org/10.1155/2013/748683.

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Fluids subject to thermal gradients produce complex behaviors that arise from the competition with gravitational effects. Although such sort of systems have been widely studied in the literature for simple (Newtonian) fluids, the behavior of viscoelastic fluids has not been explored thus far. We present a theoretical study of the dynamics of a Maxwell viscoelastic fluid in a closed-loop thermosyphon. This sort of fluid presents elastic-like behavior and memory effects. We study the asymptotic properties of the fluid inside the thermosyphon and the exact equations of motion in the inertial mani

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2

Azuma, Hisao. "Fluid Behavior in Microgvavity." Journal of the Society of Mechanical Engineers 97, no. 910 (1994): 764–66. http://dx.doi.org/10.1299/jsmemag.97.910_764.

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3

ROSENFELD, NICHOLAS, NORMAN M. WERELEY, RADHAKUMAR RADAKRISHNAN, and TIRULAI S. SUDARSHAN. "BEHAVIOR OF MAGNETORHEOLOGICAL FLUIDS UTILIZING NANOPOWDER IRON." International Journal of Modern Physics B 16, no. 17n18 (2002): 2392–98. http://dx.doi.org/10.1142/s0217979202012414.

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Iron nanopowders for use in magnetorheological (MR) fluids were synthesized using a Microwave Plasma Synthesis technique developed at Materials Modification Inc (Fairfax VA). Transmission electron microscopy and surface area analysis measured iron particle size at 15–25 nm. The nanopowders were mixed into hydraulic oil to create nano-scale MR fluid. A micro-scale fluid was created using 45 μm iron particles as well as a hybrid fluid using a 50/50 mix of micro- and nanoparticles. All three fluids had a solids loading of 60% (w/w or weight by weight fraction). The fluids were tested in a flow mo

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4

Skadsem, Hans Joakim, Amare Leulseged, and Eric Cayeux. "Measurement of Drilling Fluid Rheology and Modeling of Thixotropic Behavior." Applied Rheology 29, no. 1 (2019): 1–11. http://dx.doi.org/10.1515/arh-2019-0001.

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Abstract Drilling fluids perform a number of important functions during a drilling operation, including that of lifting drilled cuttings to the surface and balancing formation pressures. Drilling fluids are usually designed to be structured fluids exhibiting shear thinning and yield stress behavior, and most drilling fluids also exhibit thixotropy. Accurate modeling of drilling fluid rheology is necessary for predicting friction pressure losses in the wellbore while circulating, the pump pressure needed to resume circulation after a static period, and how the fluid rheology evolves with time w

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5

Bayatian, Majid, Mohammad Reza Ashouri, and Rouhallah Mahmoudkhani. "Flow Behavior Simulation with Computational Fluid Dynamics in Spray Tower Scrubber." International Journal of Environmental Science and Development 7, no. 3 (2016): 181–84. http://dx.doi.org/10.7763/ijesd.2016.v7.764.

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6

Chen, Dilin, Jie Li, Haiwen Chen, Lai Zhang, Hongna Zhang, and Yu Ma. "Electroosmotic Flow Behavior of Viscoelastic LPTT Fluid in a Microchannel." Micromachines 10, no. 12 (2019): 881. http://dx.doi.org/10.3390/mi10120881.

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In many research works, the fluid medium in electroosmosis is considered to be a Newtonian fluid, while the polymer solutions and biological fluids used in biomedical fields mostly belong to the non-Newtonian category. Based on the finite volume method (FVM), the electroosmotic flow (EOF) of viscoelastic fluids in near-neutral (pH = 7.5) solution considering four ions (K+, Cl−, H+, OH−) is numerically studied, as well as the viscoelastic fluids’ flow characteristics in a microchannel described by the Linear Phan-Thien–Tanner (LPTT) constitutive model under different conditions, including the e

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7

HU, WEI, and NORMAN M. WERELEY. "BEHAVIOR OF MR FLUIDS AT HIGH SHEAR RATE." International Journal of Modern Physics B 25, no. 07 (2011): 979–85. http://dx.doi.org/10.1142/s0217979211058535.

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The high shear rate behavior of MR fluids is investigated using a concentric rotational cylinder viscometer fabricated in-house. The rotational cylinder viscometer is designed such that a high shear rate of up to 30,000 s-1 can be applied to the MR fluid in a pure shear flow mode. As a comparison, the maximum shear rate of a commercially available parallel disk type rheometer is only up to 1,000 s-1. To determine the shear rate of the MR fluid in the viscometer, an exact expression between torque and angular velocity is established. The yield stress and viscosity of the MR fluid is determined

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8

Papautsky, Ian, John Brazzle, Timothy Ameel, and A. Bruno Frazier. "Laminar fluid behavior in microchannels using micropolar fluid theory." Sensors and Actuators A: Physical 73, no. 1-2 (1999): 101–8. http://dx.doi.org/10.1016/s0924-4247(98)00261-1.

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9

Hou, Chien-Yuan. "Fluid Dynamics and Behavior of Nonlinear Viscous Fluid Dampers." Journal of Structural Engineering 134, no. 1 (2008): 56–63. http://dx.doi.org/10.1061/(asce)0733-9445(2008)134:1(56).

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10

TANIGUCHI, Shoji. "Behavior of Particles in Fluid." Tetsu-to-Hagane 75, no. 1 (1989): 187–88. http://dx.doi.org/10.2355/tetsutohagane1955.75.1_187.

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11

Zschunke, F., R. Rivas, and P. O. Brunn. "Temperature Behavior of Magnetorheological Fluids." Applied Rheology 15, no. 2 (2005): 116–21. http://dx.doi.org/10.1515/arh-2005-0007.

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AbstractMagnetorheological fluids (MRFs) show a high but reversible rise of the viscosity upon application of an external magnetic field. This effect can be utilized in controllable friction dampers where the MR fluid flows through a gap with a adjustable magnetic field. The change in the magnitude of the magnetic field leads to a change of the viscosity of the fluid which in turn effects the pressure drop in the system. So the damping force can be controlled by the magnitude of the external magnetic field. This energy dissipation leads to a rise of the damper temperature. For designing those

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12

Aoshima, Yuki, and Hiroaki Hasegawa. "OS23-2 The Behavior of a Non-Circular Synthetic Jet Issued into a Turbulent Boundary Layer(Thermo-fluid dynamics(1),OS23 Thermo-fluid dynamics,FLUID AND THERMODYNAMICS)." Abstracts of ATEM : International Conference on Advanced Technology in Experimental Mechanics : Asian Conference on Experimental Mechanics 2015.14 (2015): 279. http://dx.doi.org/10.1299/jsmeatem.2015.14.279.

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13

Gozalpour, F., A. Danesh, D. H. Tehrani, A. C. Todd, and B. Tohidi. "Predicting Reservoir Fluid Phase and Volumetric Behavior From Samples Contaminated With Oil-Based Mud." SPE Reservoir Evaluation & Engineering 5, no. 03 (2002): 197–205. http://dx.doi.org/10.2118/78130-pa.

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Summary The impact of sample contamination with oil-based mud filtrate on phase behavior and properties of different types of reservoir fluids, including gas condensate and volatile oil, has been investigated. Two simple methods are used to determine the uncontaminated fluid composition from contaminated samples. The capability of the methods is demonstrated against highly contaminated samples. An equation-of-state (EOS)-based method also has been developed to predict the phase and volumetric properties of the retrieved composition. The method determines the required parameters of the EOS for

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14

LIU, M. B., J. Z. CHANG, H. T. LIU, and T. X. SU. "MODELING OF CONTACT ANGLES AND WETTING EFFECTS WITH PARTICLE METHODS." International Journal of Computational Methods 08, no. 04 (2011): 637–51. http://dx.doi.org/10.1142/s0219876211002733.

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The physics of fluid–fluid–solid contact line dynamics and wetting behaviors are closely related to the inter-particle and intra-molecular hydrodynamic interactions of the concerned multiple phase system. Investigation of surface tension, contact angle, and wetting behavior using molecular dynamics (MD) is practical only on extremely small time scales (nanoseconds) and length scales (nanometers) even if the most advanced high-performance computers are used. In this article we introduce two particle methods, which are smoothed particle hydrodynamics (SPH) and dissipative particle dynamics (DPD)

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15

Kaminsky, R. D. "Predicting Single-Phase and Two-Phase Non-Newtonian Flow Behavior in Pipes." Journal of Energy Resources Technology 120, no. 1 (1998): 2–7. http://dx.doi.org/10.1115/1.2795006.

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Improved and novel prediction methods are described for single-phase and two-phase flow of non-Newtonian fluids in pipes. Good predictions are achieved for pressure drop, liquid holdup fraction, and two-phase flow regime. The methods are applicable to any visco-inelastic non-Newtonian fluid and include the effect of surface roughness. The methods utilize a reference fluid for which validated models exist. For single-phase flow, the use of Newtonian and power-law reference fluids are illustrated. For two-phase flow, a Newtonian reference fluid is used. Focus is given to shear-thinning fluids. T

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16

Li, Wen Ting. "Flow Behavior of Polymer Viscoelastic Fluid in Complex Channel." Advanced Materials Research 774-776 (September 2013): 379–82. http://dx.doi.org/10.4028/www.scientific.net/amr.774-776.379.

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A finite volume method for the numerical solution of viscoelastic flows is given. The flow of a differential Phan-Thien-Tanner (PTT) fluid through an abrupt expansion-contraction channel has been chosen as a prototype example. Through the results of numerical simulations, the contours of velocity and stream function are drawn. Numerical results show that the viscoelasticity of polymer solutions is the main factor influencing the sweep efficiency. With increasing elasticity, the flowing area in the channel is enlarged significantly, thus the area with immobile zones becomes smaller, the microco

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17

de Deus, Hilbeth P. Azikri, Guilherme S. Paez Dupim, and Claudio R. Avila da Silva. "Some Aspects over Thixotropic Fluid Behavior." Advanced Materials Research 629 (December 2012): 623–34. http://dx.doi.org/10.4028/www.scientific.net/amr.629.623.

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In this work some theoretical aspects of constitutive equations for thixotropic fluids and restrictions on their functional forms are formally discussed. In the current study a formal emphasis has been given to the structural nature of this substances. The behavior of thixotropic fluids is analyzed in terms of simple isothermal laminar shear flow.

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18

Łukaszewicz, Grzegorz. "Asymptotic behavior of micropolar fluid flows." International Journal of Engineering Science 41, no. 3-5 (2003): 259–69. http://dx.doi.org/10.1016/s0020-7225(02)00208-2.

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19

Berkowitz, Rachel. "Fluid dynamics explains ancient organism behavior." Physics Today 70, no. 12 (2017): 25. http://dx.doi.org/10.1063/pt.3.3786.

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20

McCain, William D. "Heavy Components Control Reservoir Fluid Behavior." Journal of Petroleum Technology 46, no. 09 (1994): 746–50. http://dx.doi.org/10.2118/28214-pa.

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21

TAKEUCHI, Masami, Tatsushi KAWAI, Hisao FUKUI, Hiroshi MURAKAMI, and Jiro HASEGAWA. "Fluid Behavior of Root Canal Paste." Dental Materials Journal 4, no. 1 (1985): 93–99. http://dx.doi.org/10.4012/dmj.4.93.

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22

Holder, G. D. "Phase behavior in fluid-solid systems." Fluid Phase Equilibria 29 (October 1986): 447–55. http://dx.doi.org/10.1016/0378-3812(86)85043-9.

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23

Tohver, Valeria, Angel Chan, Osamu Sakurada, and Jennifer A. Lewis. "Nanoparticle Engineering of Complex Fluid Behavior." Langmuir 17, no. 26 (2001): 8414–21. http://dx.doi.org/10.1021/la011252w.

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24

Stell, George. "Critical behavior of ionic-fluid models." Physical Review A 45, no. 10 (1992): 7628–31. http://dx.doi.org/10.1103/physreva.45.7628.

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25

Mathias, Paul M., and Suphat Watanasiri. "Some Patterns of Fluid Phase Behavior." Journal of Chemical & Engineering Data 56, no. 4 (2011): 1658–65. http://dx.doi.org/10.1021/je200004s.

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26

Vescovi, Dalila, and Stefan Luding. "Merging fluid and solid granular behavior." Soft Matter 12, no. 41 (2016): 8616–28. http://dx.doi.org/10.1039/c6sm01444e.

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27

Levelt Sengers, J. M. H., G. Morrison, G. Nielson, R. F. Chang, and C. M. Everhart. "Thermodynamic behavior of supercritical fluid mixtures." International Journal of Thermophysics 7, no. 2 (1986): 231–43. http://dx.doi.org/10.1007/bf00500151.

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28

Speers, R. A., K. R. Holme, M. A. Tung, and W. T. Williamson. "Drilling fluid shear stress overshoot behavior." Rheologica Acta 26, no. 5 (1987): 447–52. http://dx.doi.org/10.1007/bf01333845.

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29

Bernard, P. F., J. M. Dorlot, J. D. Bobyn, and G. Drouin. "Rheologic behavior of intracancellous bone fluid." Journal of Biomechanics 18, no. 7 (1985): 522–23. http://dx.doi.org/10.1016/0021-9290(85)90696-7.

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30

Shah, Parth, Gauranga C. samanta, and Salvatore Capozziello. "Qualitative behavior of cosmological models combining various matter fields." International Journal of Modern Physics A 33, no. 18n19 (2018): 1850116. http://dx.doi.org/10.1142/s0217751x18501166.

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The late time accelerated expansion of the universe can be realized using scalar fields with the given self-interacting potentials. Here, we consider a straightforward approach where a three cosmic fluid mixture is assumed. The fluids are standard matter perfect fluid, dark matter, and a scalar field with the role of dark energy. A dynamical system analysis is developed in this context. A central role is played by the equation of state [Formula: see text] which determines the acceleration phase of the models. Determining the domination of a particular fluid at certain stages of the universe hi

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31

Chen, X. B. "Time-Dependent Rheological Behavior of Fluids For Electronics Packaging." Journal of Electronic Packaging 127, no. 4 (2005): 370–74. http://dx.doi.org/10.1115/1.2056568.

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In electronics packaging, one of the key processes is dispensing fluid materials, such as adhesive, epoxy, encapsulant, onto substrates or printed circuit boards for the purpose of surface mounting or encapsulation. In order to precisely control the dispensing process, the understanding and characterization of the flow behavior of the fluid being dispensed is very important, as the behavior can have a significant influence on the dispensing process. However, this task has proven to be very challenging due to the fact that the fluids for electronics packaging usually exhibit the time-dependent

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32

Lucking Bigué, Jean-Philippe, François Charron, and Jean-Sébastien Plante. "Squeeze-strengthening of magnetorheological fluids (part 1): Effect of geometry and fluid composition." Journal of Intelligent Material Systems and Structures 29, no. 1 (2017): 62–71. http://dx.doi.org/10.1177/1045389x17705214.

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Recent research has shown that magnetorheological fluid can undergo squeeze-strengthening when flow conditions promote filtration. While a Péclet number has been used to predict filtration in non-magnetic two-phase fluids submitted to slow compression, the approach has yet to be adapted to magnetorheological fluid behavior in order to predict the conditions leading to squeeze-strengthening behavior of magnetorheological fluid. In this article, a Péclet number is derived and adapted to the Bingham rheological model. This Péclet number is then compared to the experimental occurrence of squeeze-s

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33

SEE, HOWARD, CLINTON JOUNG, and CHARLES EKWEBELAM. "DYNAMIC BEHAVIOR AND YIELDING OF FIELD-RESPONSIVE PARTICULATE SUSPENSIONS." International Journal of Modern Physics B 21, no. 28n29 (2007): 4945–51. http://dx.doi.org/10.1142/s0217979207045876.

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We have examined the small strain response of an inverse ferrofluid system, consisting of micron-sized inert particles dispersed in a ferrofluid, which is a magnetisable liquid consisting of single domain magnetite nanoparticles. Under a magnetic field the inert particles will form elongated aggregates in the field direction, analogous to a magnetorheological fluid. It was found that the fluid appeared to have a Bingham fluid-like yield stress when analysed using the flow curve. However careful study of the behavior at very low shear rates revealed an ever decreasing shear stress. In addition,

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34

Naji, J., A. Zabihollah, and M. Behzad. "Vibration Behavior of Laminated Composite Beams Integrated with Magnetorheological Fluid Layer." Journal of Mechanics 33, no. 4 (2016): 417–25. http://dx.doi.org/10.1017/jmech.2016.90.

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AbstractVibration behavior of adaptive laminated composite beams integrated with magnetorheological (MR) fluid layer has been investigated using layerwise displacement theory. In most of the existing studies on the adaptive laminated beams with MR fluids, shear strain across the thickness of magnetorheological (MR) layer has been assumed a constant value, resulting in a constant shear stress in MR layer. However, due to the high shear deformation pattern inside MR layer, this assumption is not adequate to accurately describe the shear strain and stress in MR fluid layer. In this work a modifie

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35

Ginder, John M. "Behavior of Magnetorheological Fluids." MRS Bulletin 23, no. 8 (1998): 26–29. http://dx.doi.org/10.1557/s0883769400030785.

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In the absence of an applied magnetic field, magnetorheological (MR) fluids typically behave as nearly ideal Newtonian liquids. The application of a magnetic field induces magnetic dipole and multipole moments on each particle. The anisotropic magnetic forces between pairs of particles promote the head-to-tail alignment of the moments and draws the particles into proximity. These attractive interparticle forces lead to the formation of chains, columns, or more complicated networks of particles aligned with the direction of the magnetic field. When these structures are deformed mechanically, ma

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36

Mishra, Manish, P. K. Das, and Sunil Sarangi. "Transient Behavior of Crossflow Heat Exchangers With Longitudinal Conduction and Axial Dispersion." Journal of Heat Transfer 126, no. 3 (2004): 425–33. http://dx.doi.org/10.1115/1.1738422.

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Transient temperature response of the crossflow heat exchangers with finite wall capacitance and both fluids unmixed is investigated numerically for step, ramp and exponential perturbations provided in hot fluid inlet temperature. Effect of two-dimensional longitudinal conduction in separating sheet and axial dispersion in fluids on the transient response has been investigated. Conductive heat transport due to presence of axial dispersion in fluids have been analyzed in detail and shown that presence of axial dispersion in both of the fluid streams neutralizes the total conductive heat transpo

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37

Hsu, C. H., S. Y. Hu, K. Y. Kung, C. C. Kuo, and C. C. Chang. "A Study on the Flow Patterns of a Second Grade Viscoe-Lastic Fluid Past a Cavity in a Horizontal Channel." Journal of Mechanics 29, no. 2 (2012): 207–15. http://dx.doi.org/10.1017/jmech.2012.143.

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AbstractThis paper studies the behavior of second grade viscoelastic fluid past a cavity in a horizontal channel. The effects of Reynolds number, fluid elasticity and the aspect ratio of the cavity on the flow field are simulated numerically. The equations are converted into the vorticity and stream function equations. The solution is obtained by the finite difference method.The behavior of viscoelastic fluids is quite different from the Newtonian fluid, due to the effects of fluid elasticity. Only one flow pattern appears when the Newtonian fluid past the cavity. However, three kinds of flow

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38

Wijayanti, Wahyu, Laily Isro'in, and Lina Ema Purwanti. "Analisis Perilaku Pasien Hemodialisis dalam Pengontrolan Cairan Tubuh." Indonesian Journal for Health Sciences 1, no. 1 (2017): 10. http://dx.doi.org/10.24269/ijhs.v1i1.371.

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The behavior of the fluid control in hemodialysis patients can determine the success of hemodialysis therapy. Hemodialysis patients who do not abide by controlling the fluid can develop complications such as congestive heart failure. This study aimed to identify the behavior of hemodialysis patients in the control of body fluids in the Hemodialysis Dr. Harjono Ponorogo General Hospitals. The design used is descriptive with a population of 250 hemodialysis patients in Dr. Harjono Ponorogo General Hospitals. Total sample of 38 respondents to the sampling technique used was purposive sampling. Da

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39

Marum, Daniela Martins, Maria Diná Afonso, and Brian Bernardo Ochoa. "Rheological behavior of a bentonite mud." Applied Rheology 30, no. 1 (2020): 107–18. http://dx.doi.org/10.1515/arh-2020-0108.

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Abstract Predicting drilling fluids rheology is crucial to control/optimize the drilling process and the gas extraction from drilling fluids in logging systems. A Couette viscometer measured the apparent viscosity of a bentonite mud at various shear rates and temperatures. The bentonite mud behaved as a yield-pseudoplastic fluid, and a modified Herschel-Bulkley model predicted the shear rate and temperature effects upon the shear stress. A pipe viscometer was built to seek a correlation between the mud flow rate and the pressure drop and thereby determine refined Herschel-Bulkley parameters. C

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40

Rosch, Thomas W., and Jeffrey R. Errington. "Phase Behavior of Model Confined Fluids. Influence of Substrate−Fluid Interaction Strength." Journal of Physical Chemistry B 112, no. 47 (2008): 14911–19. http://dx.doi.org/10.1021/jp804419b.

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41

Kiselev, S. B., I. G. Kostyukova, and A. A. Povodyrev. "Universal crossover behavior of fluids and fluid mixtures in the critical region." International Journal of Thermophysics 12, no. 5 (1991): 877–95. http://dx.doi.org/10.1007/bf00502413.

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42

Luo, Sheng, Jodie L. Lutkenhaus, and Hadi Nasrabadi. "Effect of Nanoscale Pore-Size Distribution on Fluid Phase Behavior of Gas-Improved Oil Recovery in Shale Reservoirs." SPE Journal 25, no. 03 (2020): 1406–15. http://dx.doi.org/10.2118/190246-pa.

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Summary The improved oil recovery (IOR) of unconventional shale reservoirs has attracted much interest in recent years. Gas injection, such as carbon dioxide (CO2) and natural gas, is one of the most considered techniques for its sweep efficiency and effectiveness in low-permeability reservoirs. However, the uncertainties of fluid phase behavior in shale reservoirs pose a great challenge in evaluating the performance of a gas-injection operation. Shale reservoirs typically have macroscale to nanoscale pore-size distribution in the porous space. In fractures and macropores, the fluid shows bulk

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43

Ross, Michael G., and Mark J. M. Nijland. "Development of ingestive behavior." American Journal of Physiology-Regulatory, Integrative and Comparative Physiology 274, no. 4 (1998): R879—R893. http://dx.doi.org/10.1152/ajpregu.1998.274.4.r879.

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Swallowing represents a primary physiological function that provides for the ingestion of food and fluid. In precocial species, swallowing activity likely develops in utero to provide for a functional system during the neonatal period. The chronically instrumented ovine fetal preparation has provided the opportunity for recent advances in understanding the regulation of in utero swallowing activity. The near-term ovine fetus swallows fluid volumes (100–300 ml/kg) that are markedly greater, per body weight, than that of the adult (40–60 ml/kg). Spontaneous in utero swallowing and ingestive beha

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44

Harstad, K., and J. Bellan. "Isolated fluid oxygen drop behavior in fluid hydrogen at rocket chamber pressures." International Journal of Heat and Mass Transfer 41, no. 22 (1998): 3537–50. http://dx.doi.org/10.1016/s0017-9310(98)00049-0.

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45

Novotný, Jakub, and František Foret. "Fluid manipulation on the micro-scale: Basics of fluid behavior in microfluidics." Journal of Separation Science 40, no. 1 (2016): 383–94. http://dx.doi.org/10.1002/jssc.201600905.

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46

Weissburg, MJ. "The fluid dynamical context of chemosensory behavior." Biological Bulletin 198, no. 2 (2000): 188–202. http://dx.doi.org/10.2307/1542523.

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47

Hashemi, S., M. M. Saadatpour, and M. R. Kianoush. "Dynamic behavior of flexible rectangular fluid containers." Thin-Walled Structures 66 (May 2013): 23–38. http://dx.doi.org/10.1016/j.tws.2013.02.001.

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48

D’Auria, Bernardo, and Gennady Samorodnitsky. "Limit Behavior of Fluid Queues and Networks." Operations Research 53, no. 6 (2005): 933–45. http://dx.doi.org/10.1287/opre.1050.0215.

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49

Frank, Katherine, Christopher Childers, Dhanadeep Dutta, et al. "Fluid uptake behavior of multifunctional epoxy blends." Polymer 54, no. 1 (2013): 403–10. http://dx.doi.org/10.1016/j.polymer.2012.11.065.

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50

Dingwell, D. B., K. U. Hess, and C. Romano. "Extremely fluid behavior of hydrous peralkaline rhyolites." Earth and Planetary Science Letters 158, no. 1-2 (1998): 31–38. http://dx.doi.org/10.1016/s0012-821x(98)00046-6.

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