Letteratura scientifica selezionata sul tema "Viscous"

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Articoli di riviste sul tema "Viscous"

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Adhikari, Sondipon. "Qualitative dynamic characteristics of a non-viscously damped oscillator". Proceedings of the Royal Society A: Mathematical, Physical and Engineering Sciences 461, n. 2059 (16 giugno 2005): 2269–88. http://dx.doi.org/10.1098/rspa.2005.1485.

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This paper considers the linear dynamics of a single-degree-of-freedom non-viscously damped oscillator. It is assumed that the non-viscous damping force depends on the history of velocity via a convolution integral over an exponentially decaying kernel function. Classical qualitative dynamic properties known for viscously damped oscillators have been generalized to such non-viscously damped oscillators. The following questions of fundamental interest have been addressed: (i) under what conditions can a non-viscously damped oscillator sustain oscillatory motions? (ii) how does the natural frequency of a non-viscously damped oscillator compare with that of an equivalent undamped oscillator? and (iii) how does the decay rate compare with that of an equivalent viscously damped oscillator? Introducing two non-dimensional factors, namely, the viscous damping factor and the non-viscous damping factor, we provide answers to these questions. Wherever possible, attempts are made to relate the new results with equivalent classical results for a viscously damped oscillator.
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Kang, Jae-Hoon. "Closed-Form Exact Solutions for Viscously Damped Free and Forced Vibrations of Longitudinal and Torsional Bars". International Journal of Structural Stability and Dynamics 17, n. 08 (ottobre 2017): 1750093. http://dx.doi.org/10.1142/s0219455417500936.

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This paper studies the viscously damped free and forced vibrations of longitudinal and torsional bars. The method is exact and yields closed form solution for the vibration displacement in contrast with the well-known eigenfunction superposition (ES) method, which requires expression of the distributed forcing functions and displacement response functions as infinite series sums of free vibration eigenfunctions. The viscously damped natural frequency equation and the critical viscous damping equation are exactly derived for the bars. Then the viscously damped free vibration frequencies and corresponding damped mode shapes are calculated and plotted, aside from the undamped free vibration and corresponding mode shapes typically computed and used in vibration problems. The longitudinal or torsional amplitude versus forcing frequency curves showing the forced response to distributed loadings are plotted for various viscous damping parameters. It is found that the viscous damping affects the natural frequencies and the corresponding mode shapes of longitudinal and torsional bars, especially for the fundamental frequency.
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Irklei, V. M., G. I. Berestyuk e K. Ya Reznik. "Filtration of highly-viscous viscoses at elevated temperatures". Fibre Chemistry 18, n. 2 (1986): 111–13. http://dx.doi.org/10.1007/bf00549625.

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Coclici, Cristian, Gheorghe Moroşanu e Wolfgang L. Wendland. "On the viscous–viscous and the viscous–inviscid interactions in Computational Fluid Dynamics". Computing and Visualization in Science 2, n. 2-3 (dicembre 1999): 95–105. http://dx.doi.org/10.1007/s007910050032.

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Persaud, Donny, Josh Lepawsky e Max Liboiron. "« Viscous objects »". Techniques & culture, n. 72 (25 novembre 2019): 126–29. http://dx.doi.org/10.4000/tc.12504.

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Muronga, Azwinndini. "Viscous hydrodynamics". Journal of Physics G: Nuclear and Particle Physics 31, n. 6 (23 maggio 2005): S1035—S1039. http://dx.doi.org/10.1088/0954-3899/31/6/053.

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Bravo Medina, Sergio, Marek Nowakowski e Davide Batic. "Viscous cosmologies". Classical and Quantum Gravity 36, n. 21 (10 ottobre 2019): 215002. http://dx.doi.org/10.1088/1361-6382/ab45bb.

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John Newman. "Viscous Sublayer". Russian Journal of Electrochemistry 56, n. 3 (marzo 2020): 263–69. http://dx.doi.org/10.1134/s102319352003009x.

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Le Goff, Anne, David Quéré e Christophe Clanet. "Viscous cavities". Physics of Fluids 25, n. 4 (aprile 2013): 043101. http://dx.doi.org/10.1063/1.4797499.

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Jha, Aditya, Pierre Chantelot, Christophe Clanet e David Quéré. "Viscous bouncing". Soft Matter 16, n. 31 (2020): 7270–73. http://dx.doi.org/10.1039/d0sm00955e.

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Tesi sul tema "Viscous"

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Koulakis, John. "The viscous catenary". Pomona College, 2006. http://ccdl.libraries.claremont.edu/u?/stc,3.

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Variational techniques are used to develop a theory for the time evolution of a thin strand of viscous fluid suspended from two points. The shape of the strand is approximated to be a parabola and energy conservation is used to derive a differential equation modeling the change in height over time. Data is collected with a high resolution camera and a strobe light to obtain the position and shape of the strand over multiple intervals of time. Three very different and unexpected types of behaviors are observed depending on the initial thickness and shape of the filament. The approximation fits well with one type of behavior but variations in the thickness of the strand, and consequently in the center of mass, need to be factored in to predict the others.
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Corvera, Poiré Eugenia. "Anisotropic viscous fingering". Thesis, McGill University, 1995. http://digitool.Library.McGill.CA:80/R/?func=dbin-jump-full&object_id=29002.

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We have qualitatively explained the experiments of McCloud and Maher (McCloud and Maher (95)) for the viscous fingering problem in which an anisotropy in the surface tension parameter was imposed by engraving a grid in one of the plates of the Hele-Shaw cell. We saw the need to approach the problem in an analytical form. Therefore we decided to extend solvability theory to incorporate the effect of anisotropy. We have introduced the anisotropy through a moving boundary condition by considering an effective anisotropic surface tension with an anisotropy entering as the simplest cosine term having the right symmetry for a square lattice. We carried out the singular perturbation appropriate for the surface tension parameter assuming the length scale introduced by the anisotropy is small in comparison with the length scale introduced by the surface tension. In this sense, the perturbation can be said to be microscopic. For the case in which the surface tension has a maximum at the finger tip, our theory provides two possible solutions: one corresponding to the solution of the isotropic case and a new solution which, below a threshold of the surface tension parameter, predicts a wider finger than the isotropic solution. Intuitively, we expect the "old" solution, namely the one that does not differ from the isotropic case, to be the selected solution for large values of the surface tension parameter and we expect the new solution to be selected for small values of the surface tension parameter. This was confirmed by dynamical simulations of the interface done by David Jasnow. His simulation predicts that for the case in which the surface tension has a maximum at the finger tip, anisotropy is irrelevant for large values of the surface tension parameter. Furthermore below a threshold in this surface tension parameter, the selected finger width is systematically wider than the corresponding isotropic case. We conclude that our solvability theory together with the dynamic
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Savva, Nikos. "Viscous fluid sheets". Thesis, Massachusetts Institute of Technology, 2007. http://hdl.handle.net/1721.1/41725.

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Thesis (Ph. D.)--Massachusetts Institute of Technology, Dept. of Mathematics, 2007.
Includes bibliographical references (leaves 108-117).
We present a general theory for the dynamics of thin viscous sheets. Employing concepts from differential geometry and tensor calculus we derive the governing equations in terms of a coordinate system that moves with the film. Special attention is given to incorporating inertia and the curvature forces that arise from the thickness variations along the film. Exploiting the slenderness of the film, we assume that the transverse fluid velocity is small compared to the longitudinal one and perform a perturbation expansion to obtain the leading order equations when the center-surface that defines the coordinate system is parametrized by lines of curvature. We then focus on the dynamics of flat film rupture, in an attempt to gain some insights into the sheet breakup and its fragmentation into droplets. By combining analytical and numerical methods, we extend the prior work on the subject and compare our numerical simulations with experimental work reported in the literature.
by Nikos Savva.
Ph.D.
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Beeson-Jones, Timothy. "Controlling viscous fingering". Thesis, University of Cambridge, 2018. https://www.repository.cam.ac.uk/handle/1810/275358.

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Viscous fingering occurs when one fluid displaces another fluid of a greater viscosity in a porous medium or a Hele-Shaw cell. Linear stability analysis is used to predict methods of suppressing instability. Then, experiments in which nonlinear growth dominates pattern formation are analysed to explore the nonlinear impact of strategies of suppressing finger growth. Often, chemical treatment fluid is injected into oil reservoirs in order to prevent sand production. This treatment fluid is usually followed by water injection to clean up the well. We explore the potential for viscous instability of the interface between the treatment fluid and the water, and also the treatment fluid and the oil, as a function of the volume of treatment fluid and the injection rate and viscosity ratios of the different fluids. For a given volume of treatment fluid and a given injection rate, we find the optimal viscosity of the treatment fluid to minimise the viscous instability. In the case of axisymmetric injection, the stabilisation associated with the azimuthal stretching of modes leads to a further constraint on the optimisation of the viscosity. In the case of oil production, polymers may be added to the displacing water in order to reduce adverse viscosity gradients. We also explore the case in which these polymers have a time-dependent viscosity, for example through the slow release from encapsulant. We calculate the injection flow rate profile that minimises the final amplitude of instability in both rectilinear and axisymmetric geometries. In a development of the model, we repeat the calculation for a shear-thinning rheology. Finally, experiments are analysed in which the nonlinear growth of viscous fingers develops to test the influence of different injection profiles on the development of instability. Diffusion Limited Aggregation (DLA) simulations are performed for comparison. In all cases, the evolving pattern has a saturation distribution, with an inner zone in which the fingers are static and an outer zone in which the fingers advance and grow. In the very centre of the viscous fingering patterns, there is a small fully-saturated region. In the experiments, the mass distribution in the inner zone varies with radius as a power law which relates to the fractal dimension for the analogue DLA simulations. In the outer region the saturation decreases linearly with radius. The radius of the inner frozen zone is approximately 2/3 of the outer radius in the cases of DLA and -- after a period of evolution -- the viscous fingering experiments. This allows the radial extents of the inner and outer zones to be predicted. The ratio of each radius to the extent of the fully-saturated region is independent of the injection profile and corresponds to values for DLA.
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Siklos, Malin. "Aspects of viscous shocks". Doctoral thesis, KTH, Numerical Analysis and Computer Science, NADA, 2004. http://urn.kb.se/resolve?urn=urn:nbn:se:kth:diva-89.

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This thesis consists of an introduction and five papers concerning different numerical and mathematical aspects of viscous shocks.

Hyperbolic conservation laws are used to model wave motion and advect- ive transport in a variety of physical applications. Solutions of hyperbolic conservation laws may become discontinuous, even in cases where initial and boundary data are smooth. Shock waves is one important type of discontinu- ity. It is also interesting to study the corresponding slightly viscous system, i.e., the system obtained when a small viscous term is added to the hyper- bolic system of equations. By a viscous shock we denote a thin transition layer which appears in the solution of the slightly viscous system instead of a shock in the corresponding purely hyperbolic problem.

A slightly viscous system, a so called modified equation, is often used to model numerical solutions of hyperbolic conservation laws and their beha- vior in the vicinity of shocks. Computations presented elsewhere show that numerical solutions of hyperbolic conservation laws obtained by higher order accurate shock capturing methods in many cases are only first order accurate downstream of shocks. We use a modified equation to model numerical solu- tions obtained by a generic second order shock capturing scheme for a time dependent system in one space dimension. We present analysis that show how the first order error term is related to the viscous terms and show that it is possible to eliminate the first order downstream error by choosing a special viscosity term. This is verified in computations. We also extend the analysis to a stationary problem in two space dimensions.

Though the technique of modified equation is widely used, rather little is known about when (for what methods etc.) it is applicable. The use of a modified equation as a model for a numerical solution is only relevant if the numerical solution behaves as a continuous function. We have experimentally investigated a range of high resolution shock capturing methods. Our experiments indicate that for many of the methods there is a continuous shock profile. For some of the methods, however, this not the case. In general the behavior in the shock region is very complicated.

Systems of hyperbolic conservation laws with solutions containing shock waves, and corresponding slightly viscous equations, are examples where the available theoretical results on existence and uniqueness of solutions are very limited, though it is often straightforward to find approximate numerical solu- tions. We present a computer-assisted technique to prove existence of solu- tions of non-linear boundary value ODEs, which is based on using an approx- imate, numerical solution. The technique is applied to stationary solutions of the viscous Burgers' equation.We also study a corresponding method suggested by Yamamoto in SIAM J. Numer. Anal. 35(5)1998, and apply also this method to the viscous Burgers' equation.

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Siklosi, Malin. "Aspects of viscous shocks". Doctoral thesis, Stockholm, 2004. http://urn.kb.se/resolve?urn=urn:nbn:se:kth:diva-3905.

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Crosby, Andrew. "Buoyancy-driven viscous flows". Thesis, University of Cambridge, 2013. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.648304.

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Chakrabarti, Brato. "Catenaries in Viscous Fluid". Thesis, Virginia Tech, 2015. http://hdl.handle.net/10919/53832.

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Slender structures in fluid flow exhibit a variety of rich behaviors. Here we study the equilibrium shapes of perfectly flexible strings that are moving with a uniform velocity and axial flow in viscous fluid. The string is acted upon by local, anisotropic, linear drag forces and a uniform body force. Generically, the configurations of the string are planar, and we provide analytical expressions for the equilibrium shapes of the string as a first order five parameter dynamical system for the tangential angle of the body ($theta$). Phase portraits in the angle-curvature ($theta,partial_s theta$) plane are generated, that can be shown to be $pi$ periodic after appropriate scaling and reflection operations. The rich parameter space allows for different kinds of phase portraits that give rise to a variety of curve geometries. Some of these solutions are unstable due to the presence of compressive stresses. Special cases of the problem include sedimenting filaments, dynamic catenaries, and towed strings. We also discuss equilibrium configurations of towed cables and other relevant problems with fixed boundary conditions. Special cases of the boundary value problem involve towing of neutrally buoyant cables and strings with pure axial flow between two fixed points.
Master of Science
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Panda, Satyananda. "The dynamics of viscous fibers". [S.l.] : [s.n.], 2006. http://deposit.ddb.de/cgi-bin/dokserv?idn=979183138.

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Stropky, Dave. "A viscous-inviscid interaction procedure". Thesis, University of British Columbia, 1988. http://hdl.handle.net/2429/28521.

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A new viscous-inviscid semi-inverse (VISI) interaction method has been developed for predicting the flow field arising from a combination of inviscid potential flow and viscous flow. The technique involves matching the bounding velocities for each region by iteratively solving for the displacement thickness, δ*(x). The formula used to update δ*(x) after each iteration is generated by linearly perturbing the governing equations. Application of the VISI procedure to predict the unseparated flow past a flat plate gives excellent results, producing numerical solutions essentially indistinguishable from the appropriate analytical solution in less than 0.5 seconds of CPU time on an Amdahl 5850 computer. Application of the technique to external flow over a backward facing step (BFS) indicates that the region of strong interaction between the viscous and inviscid flows is much larger than reported for internal flow. Calculated reattachment lengths, LR, are clearly influenced by the thickness of the boundary layer upstream of the step, thicker boundary layers producing longer reattachment lengths. Good accuracy is achieved for a relatively coarse distribution of control points, and rapid convergence (< 2 seconds on the Amdahl 5850) usually occurs. Finite-difference predictions using an elliptic code (TEACH-T), modified at the outer boundary to simulate external flow, have also been made for the BFS, largely as a basis of comparison for the VISI results. Comparison of results for the two models (VISI and TEACH) gives similar trends in LR as a function of Rh and x₈, (a measure of the displacement thickness at the step). The values of LR obtained with the VISI method, however, are 15-80% longer than those from TEACH. Direct comparison with experiments is difficult because the experimental data does not clearly identify the effects of x₈, in the resulting values of LR. Trends appear to be the same for all computed and observed cases however. Disagreement between the VISI and TEACH results is thought to be due to a combination of neglecting velocities in the recirculation region in the VISI model, and numerical error and inaccurate boundary conditions in the TEACH code.
Applied Science, Faculty of
Mechanical Engineering, Department of
Graduate
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Libri sul tema "Viscous"

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Mehmood, Ahmer. Viscous Flows. Cham: Springer International Publishing, 2017. http://dx.doi.org/10.1007/978-3-319-55432-7.

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Viscous flow. New York: McGraw-Hill, 1990.

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R, Ockendon J., a cura di. Viscous flow. Cambridge: Cambridge University Press, 1995.

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Viscous flow. Maidenhead: McGraw Hill, 1990.

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Stern, Frederick. Viscous-inviscid interaction with higher-order viscous-flow equations. Iowa City, Iowa: Iowa Institute of Hydraulic Research, The University of Iowa, 1986.

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Brebbia, Carlos A., a cura di. Viscous Flow Applications. Berlin, Heidelberg: Springer Berlin Heidelberg, 1989. http://dx.doi.org/10.1007/978-3-642-83683-1.

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Langlois, William E., e Michel O. Deville. Slow Viscous Flow. Cham: Springer International Publishing, 2014. http://dx.doi.org/10.1007/978-3-319-03835-3.

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Constantinescu, V. N. Laminar Viscous Flow. New York, NY: Springer New York, 1995. http://dx.doi.org/10.1007/978-1-4612-4244-4.

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Laminar viscous flow. New York: Springer, 1995.

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Viscous fluid flow. 2a ed. New York: McGraw-Hill, 1991.

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Capitoli di libri sul tema "Viscous"

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Gooch, Jan W. "Viscous". In Encyclopedic Dictionary of Polymers, 800. New York, NY: Springer New York, 2011. http://dx.doi.org/10.1007/978-1-4419-6247-8_12615.

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Mehmood, Ahmer. "Viscous Flow Due to Moving Continuous Surfaces". In Viscous Flows, 3–11. Cham: Springer International Publishing, 2017. http://dx.doi.org/10.1007/978-3-319-55432-7_1.

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Mehmood, Ahmer. "Axially Symmetric Non-similar Flows". In Viscous Flows, 143–61. Cham: Springer International Publishing, 2017. http://dx.doi.org/10.1007/978-3-319-55432-7_10.

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Mehmood, Ahmer. "Time-Dependent Non-similarity". In Viscous Flows, 163–77. Cham: Springer International Publishing, 2017. http://dx.doi.org/10.1007/978-3-319-55432-7_11.

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Mehmood, Ahmer. "Turbulent Flow Due to Moving Continuous Surfaces". In Viscous Flows, 181–93. Cham: Springer International Publishing, 2017. http://dx.doi.org/10.1007/978-3-319-55432-7_12.

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Mehmood, Ahmer. "Governing Equations". In Viscous Flows, 13–21. Cham: Springer International Publishing, 2017. http://dx.doi.org/10.1007/978-3-319-55432-7_2.

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Mehmood, Ahmer. "The Concept of Self-similarity". In Viscous Flows, 23–32. Cham: Springer International Publishing, 2017. http://dx.doi.org/10.1007/978-3-319-55432-7_3.

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Mehmood, Ahmer. "Solution Techniques". In Viscous Flows, 33–41. Cham: Springer International Publishing, 2017. http://dx.doi.org/10.1007/978-3-319-55432-7_4.

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Mehmood, Ahmer. "The Criterion of Self-similarity for Wall Velocities". In Viscous Flows, 45–74. Cham: Springer International Publishing, 2017. http://dx.doi.org/10.1007/978-3-319-55432-7_5.

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Mehmood, Ahmer. "Viscous Flow Due to Accelerated/Decelerated Stretching Surfaces". In Viscous Flows, 75–99. Cham: Springer International Publishing, 2017. http://dx.doi.org/10.1007/978-3-319-55432-7_6.

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Atti di convegni sul tema "Viscous"

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Li, Peiwen, Gosia Pawlowska e Wenbo Zhu. "Viscous Catenary". In ACADIA 2020: Distributed Proximities. ACADIA, 2020. http://dx.doi.org/10.52842/conf.acadia.2020.2.170.

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Shirvanee, Lily, e Glorianna Davenport. "The Viscous Display". In the 2nd international conference. New York, New York, USA: ACM Press, 2004. http://dx.doi.org/10.1145/988834.988879.

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GREENE, GEORGE. "Viscous induced drag". In 6th Applied Aerodynamics Conference. Reston, Virigina: American Institute of Aeronautics and Astronautics, 1988. http://dx.doi.org/10.2514/6.1988-2550.

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Abdelgawad, M., I. Hassan, N. Esmail e P. Phutthavong. "Multistage Viscous Micropumps". In ASME 2004 2nd International Conference on Microchannels and Minichannels. ASMEDC, 2004. http://dx.doi.org/10.1115/icmm2004-2407.

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The viscous micropump consists of a cylinder placed eccentrically inside a microchannel, where the rotor axis is perpendicular to the channel axis. When the cylinder rotates, a net force is transferred to the fluid due to the unequal shear stresses on the upper and lower surfaces of the rotor. Consequently, this causes the surrounding fluid in the channel to displace towards the microchannel outlet. The simplicity of the viscous micropump renders it ideal for micro pumping, however, previous studies have shown that its performance is still less than what is required for various applications. The performance of the viscous micropump, in terms of flow rate, pressure head and efficiency, may be enhanced by implementing more than one rotor into the configuration. The present study will numerically investigate the performance of various configurations of the viscous micropumps with multiple rotors, namely the dual-horizontal rotor, the triple-horizontal rotor, the symmetrical-dual-vertical rotor, and the 8-shaped dual-vertical rotor. The development of drag force with time, as well as the viscous resisting torque on the cylinders were studied. In addition, the corresponding drag and moment coefficients were calculated. Results show that the symmetrical-dual-vertical rotor configuration yields the best efficiency, and generates the highest flow rate. The steady state performance of the single-stage micropump was compared with the available experimental and numerical data, and was found to be in very good agreement. This work provides a foundation for future research on the subject of fluid phenomena in viscous micropumps.
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Blas, Diego, Stefan Floerchinger, Mathias Garny, Nikolaos Tetradis e Urs Achim Wiedemann. "Viscous dark matter". In Proceedings of the MG14 Meeting on General Relativity. WORLD SCIENTIFIC, 2017. http://dx.doi.org/10.1142/9789813226609_0278.

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Bergou, Miklós, Basile Audoly, Etienne Vouga, Max Wardetzky e Eitan Grinspun. "Discrete viscous threads". In ACM SIGGRAPH 2010 papers. New York, New York, USA: ACM Press, 2010. http://dx.doi.org/10.1145/1833349.1778853.

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Su, Jichao. "A Viscous-Inviscid Zonal Method for Compressible and Incompressible Viscous Flows". In 17th AIAA Computational Fluid Dynamics Conference. Reston, Virigina: American Institute of Aeronautics and Astronautics, 2005. http://dx.doi.org/10.2514/6.2005-5340.

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Su, Jichao. "Calculation of Incompressible Viscous Flows by a Viscous-Inviscid Splitting Method". In World Aviation Congress & Exposition. 400 Commonwealth Drive, Warrendale, PA, United States: SAE International, 2001. http://dx.doi.org/10.4271/2001-01-2977.

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CHANG, CHAU-LYAN, e CHARLES MERKLE. "Viscous swirling nozzle flow". In 27th Aerospace Sciences Meeting. Reston, Virigina: American Institute of Aeronautics and Astronautics, 1989. http://dx.doi.org/10.2514/6.1989-280.

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Beliveau, Dennis. "Waterflooding Viscous Oil Reservoirs". In SPE Indian Oil and Gas Technical Conference and Exhibition. Society of Petroleum Engineers, 2008. http://dx.doi.org/10.2118/113132-ms.

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Rapporti di organizzazioni sul tema "Viscous"

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Stix, T. H., e M. Ono. Viscous current drive. Office of Scientific and Technical Information (OSTI), aprile 1985. http://dx.doi.org/10.2172/5761611.

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Stern, Fred. Unsteady Viscous Propusor Hydrodynamics. Fort Belvoir, VA: Defense Technical Information Center, settembre 1994. http://dx.doi.org/10.21236/ada300213.

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Reshotko, Eli. Time-Dependent Hypersonic Viscous Interactions. Fort Belvoir, VA: Defense Technical Information Center, giugno 1987. http://dx.doi.org/10.21236/ada185764.

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JOSEPH, DANIEL D. LUBRICATED TRANSPORT OF VISCOUS FLUIDS. Office of Scientific and Technical Information (OSTI), giugno 2004. http://dx.doi.org/10.2172/825229.

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Shen, S. F. Unsteady Viscous Flows Over Moving Body. Fort Belvoir, VA: Defense Technical Information Center, agosto 1988. http://dx.doi.org/10.21236/ada200269.

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Rothmayer, A. P. Nonlinear Stability of Unsteady Viscous Flow. Fort Belvoir, VA: Defense Technical Information Center, aprile 1995. http://dx.doi.org/10.21236/ada294931.

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Mohanty, Kishore. Chemical Methods for Ugnu Viscous Oils. Office of Scientific and Technical Information (OSTI), marzo 2012. http://dx.doi.org/10.2172/1048103.

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Scott Misture. Viscous Glass Sealants for SOFC Applications. Office of Scientific and Technical Information (OSTI), settembre 2012. http://dx.doi.org/10.2172/1062658.

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Gomon, M. Experimental study of highly viscous impinging jets. Office of Scientific and Technical Information (OSTI), dicembre 1998. http://dx.doi.org/10.2172/296715.

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Romatschke, Paul. A realistic 3+1D Viscous Hydro Algorithm. Office of Scientific and Technical Information (OSTI), maggio 2015. http://dx.doi.org/10.2172/1233593.

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