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A multi-resolution discontinuous galerkin method for unsteady compressible flowsShelton, Andrew Brian January 2008 (has links)
Thesis (Ph.D.)--Aerospace Engineering, Georgia Institute of Technology, 2009. / Committee Chair: Smith, Marilyn; Committee Co-Chair: Zhou, Hao-Min; Committee Member: Dieci, Luca; Committee Member: Menon, Suresh; Committee Member: Ruffin, Stephen
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Non-isothermal characterization of squeezed thin films in the presence of biofluids and suspended ultrafine particlesKhaled, Abdul Rahim Assaad, January 2003 (has links)
Thesis (Ph. D.)--Ohio State University, 2003. / Title from first page of PDF file. Document formatted into pages; contains xix, 172 p.; also includes graphics. Includes bibliographical references (p. 168-172).
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Tip clearance and angle of attack effects upon the unsteady response of a vibrating flat plate in crossflow /Lewis, Daniel Joseph, January 1993 (has links)
Thesis (M.S.)--Virginia Polytechnic Institute and State University, 1993. / Vita. Abstract. Includes bibliographical references (leaves 47-50). Also available via the Internet.
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Some unsteady problems in fluid dynamicsCzaykowski, Jerzy T. January 1970 (has links)
No description available.
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Aerodynamic stability of road vehicles in side winds and gustsMullarkey, Seamus Paul January 1990 (has links)
No description available.
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Unsteady Skin-Friction Measurements on a Maneuvering Darpa2 Suboff ModelHosder, Serhat 22 June 2001 (has links)
Steady and unsteady flow over a generic Suboff submarine model is studied. The skin-friction magnitudes are measured by using hot-film sensors each connected to a constant temperature anemometer. The local minima in the skin-friction magnitudes are used to obtain the separation locations. Steady static pressure measurements on the model surface are performed at 10° and 20° angles of attack. Steady and unsteady results are presented for two model configurations: barebody and sail-on-side case. The dynamic plunge-pitch-roll model mount (DyPPiR) is used to simulate the pitchup maneuvers. The pitchup maneuver is a linear ramp from 1° to 27° in 0.33 seconds. All the tests are conducted at ReL=5,500,000 with a nominal wind tunnel speed of 42.7±1 m/s. Steady results show that the flow structure on the leeward side of the barebody can be characterized by the crossflow separation. In the sail-on-side case, the separation pattern of the non-sail region follow the barebody separation trend closely. The flow on the sail side is strongly affected by the presence of the sail and the separation pattern is different from the crossflow separation. The flow in the vicinity of the sail-body junction is dominated by the horseshoe type separation. Unsteady results of the barebody and the non-sail region of the sail-on-side case show significant time lags between unsteady and steady crossflow separation locations. These effects produce the difference in separation topology between the unsteady and steady flowfields. A first-order time lag model approximates the unsteady separation locations reasonably well and time lags are obtained by fitting the model equation with the experimental data. The unsteady separation pattern of the sail side does not follow the quasi-steady data with a time lag and the unsteady separation structure is different from the unsteady crossflow separation topology observed for the barebody and the non-sail region of the sail-on-side case. / Master of Science
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Mathematical Model for Estimating Transient Pressure Surges in Cryogenic Liquid-Vapor SystemsPfister, Philippe 01 January 1983 (has links) (PDF)
Numerical treatments have become the most accurate methods for transient liquid flows analysis. Based on a computer code provided by NASA/KSC, this paper presents two simulations of cryogenic transfer systems. Experimental data originated from the Space Shuttle Liquid Oxygen Servicing were obtained during drain flows. Two sets of data (pressure at various locations versus time) corresponding to a drain stop and a drain initiation were used for a comparison with the predicted pressures. The first test case was a single-phase flow whereas the second one was associated with liquid-column separation and vapor cavity collapse. Major modifications were made to the computer program for two-phase flow treatments. Encouraging results have been obtained validating the model and opening new perspectives for future work.
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A Planar Laser-induced Fluorescence Study on the Effects of Unsteadiness and Fuel Lewis Number in Hydrogen Laminar Diffusion FlamesChaos, Marcos 01 January 2003 (has links) (PDF)
Studies on the effect of transport properties coupled with the interaction of fluid dynamics and combustion in acoustically forced laminar hydrogen jet diffusion flames have been performed using the planar laser-induced fluorescence (PLIF) technique. These unsteady diffusion flames are of particular interest because they are reproducible turbulent-like events that can be investigated to gain insight into turbulent combustion. Results reported herein add to the ongoing effort of understanding the complex transport processes taking place in the flames encountered in most modern heat-producing and power-producing devices.
Fuel transport properties (i .e. fuel Lewis number, LeF) were varied by fuel dilution with various levels of helium (He) or argon (Ar). The fuel stream ofBurkeSchumann type hydrogen flames was acoustically excited by using a loudspeaker and the two-dimensional OH and temperature fields were measured. PLIF measurements were performed using an intricate two-laser, two-camera system; digital image analysis was implemented to reduce the large image data set obtained.
The temperature of the unsteady flames departed significantly from the steadystate temperature as predicted by previous researchers. It was found that, regardless of LeF, unsteady He-diluted flames had maximum flame temperatures at some point during the speaker -oscillation that were always higher than the maximum temperatures of the H2-Ar flames. This was contrary to the trends seen in steady flames. An increased H2 mass flux to the flame zone in the unsteady H2-He flames was the reason for this observation since mass diffusion becomes important in the driven flames due to increased mass gradients and the difference in diffusivity of hydrogen in the diluents used.
Low turbulence intensities (i.e.low frequency) allowed the flames to respond steadily to the changing flowfield. The structure of the reaction zone of unsteady flames at this low frequency was altered (i.e. stretched or compressed) slightly and, in general, these flames resembled the steady flames structurally. At high frequency, however, the flames responded to the imposed flow oscillation by considerable reaction zone stretch/compression. Results obtained from the present experiments suggest that, depending on the Lewis number, the flame temperature responds differently to the stretch imparted on the flame by the unsteady flowfield. These Lewis number effects were evidenced by both the low and high frequency flames, however, they were most obvious in the high frequency cases. The temperature of flames with LeF ~ l increased/decreased when the reaction zone thickened/thinned. On the other hand, flames with LeF < l increased/decreased in temperature when the reaction zone thinned/thickened. These trends competed with the thermal and mass transport processes present in the high-curvature regions of the flames.
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A non linear frequency domain-spectral difference scheme for unsteady periodic flows /Cagnone, Jean-Sébastien January 2008 (has links)
No description available.
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Rotor/Fuselage Unsteady Interactional Aerodynamics: A New Computational ModelBoyd, David Douglas Jr. 13 August 1999 (has links)
A new unsteady rotor/fuselage interactional aerodynamics model has been developed. This model loosely couples a Generalized Dynamic Wake Theory (GDWT) to a Navier-Stokes solution procedure. This coupling is achieved using a newly developed unsteady pressure jump boundary condition in the Navier-Stokes model. The new unsteady pressure jump boundary condition models each rotor blade as a moving pressure jump which travels around the rotor azimuth =and is applied between two adjacent planes in a cylindrical, non-rotating grid. Comparisons are made between predictions using this new model and experiments for an isolated rotor and for a coupled rotor/fuselage configuration. / Ph. D.
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