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Experimental study of ionised gases produced by shock wavesLaird, John D. January 1965 (has links)
No description available.
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An asymptotic approach for shock-wave/turbulent boundary layer interactionsSilva Freire, Atila P. January 1987 (has links)
No description available.
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Evaluation of straight and swept ramp obstacles on enhancing deflagration-to-detonation transition in pulse detonation enginesMedina, Carlos A. 12 1900 (has links)
The use of detonations to achieve thrust in pulse detonation engines (PDEs) offers significant advantages in efficiency, simplicity, and versatility. An enabling mechanism for practical PDE implementation will likely utilize an efficient deflagration-todetonation transition (DDT) process. This method simplifies detonation generation, but the required length is prohibitive in many applications and limits the frequency of repeatability. Obstacles have historically been employed to minimize the DDT distance, but often result in significant total pressure losses that degrade the delivered efficiency advantages of PDEs. This thesis explored the use of straight and swept ramp obstacles to accelerate DDT while minimizing the overall pressure losses. Computer modeling examined three-dimensional disturbances caused by such obstacles. Experimental tests measured combustion shockwave speed, flame velocity, and flame front interactions with obstacles. Evaluations were completed for several straight ramp obstacle configurations in a modeled two-dimensional flow. The placement of consecutive ramps resulted in flame acceleration accompanied by significant pressure spikes approaching 500 psi. Although detonation was not verified across the instrumented section, experimental data prove that straight ramp obstacles successfully accelerate the DDT process. Computer modeling predicts that swept ramps may be even more effective by introducing streamwise vorticity with a relatively low pressure drop.
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Shock wave interactions with porous platesSeeraj, Sumil 08 May 2009 (has links)
The idea of creating a material or barrier that attenuates shock and blast waves has long been investigated.
Considerable work has been performed on the interactions of shock and blast waves with various
materials. The application of permeable solids, porous materials and textiles for the attenuation and
reflection of destructive shock waves have been studied extensively. The studies presented herein
examine the interaction of shock waves and porous plates in order to ameliorate the hazardous effects of
these waves particularly in ducts or channels leading to protected areas or objects. A number of tests were
performed in an automated shock tube to determine the effects that a series of directional porous plates
had on the initial peak pressure and impulse amelioration experienced by the end wall. Mild steel test
specimens, ranging in porosity values from 6.6 % to 41.1 %, were mounted two at a time in the test
section of the shock tube. Each plate had directional properties and since four plates were used in the
study, a total of forty eight plate configurations were tested. Six pressure transducers were located along
the side of the test section and two pressure transducers were located in the end wall of the shock tube in
order to measure initial peak pressure and impulse amelioration values experienced by the end wall and to
identify the wave interactions involved in the amelioration process. Schlieren photographs were also
taken in order to investigate these wave interactions. Tests were run at three different Mach numbers viz.
1.23, 1.35 and 1.42. The separation distances between the plate specimens were varied between 30 mm
and 60 mm; however the distance between the downstream plate and the end wall was kept constant at
140mm for all tests. It was found that significant initial peak pressure and impulse amelioration was
achievable. The Back & Back plate arrangement produced the greatest initial peak pressure and impulse
amelioration with averages values of 73.7 % and 20.45 % respectively. Both the initial peak pressure and
impulse amelioration values were found to be dependant on the plate combination porosity. As the
porosity of the combination increased, the amelioration values decreased. Complementary plate
combinations produced differing results as different wave interactions occur when plate positions were
interchanged. The porosity of the combined plates were found to have an overriding influence on the end
wall initial peak pressure and impulse amelioration values when compared to the effect that plate
arrangement (i.e. geometrical influences) had. For all tests performed in this study, the time period used
for the integration of the end wall pressure traces was 9 250 μs. As an acceptable closing time for a blast
valve in a shelter’s ventilation system is approximately 4 000 μs, the impulse amelioration values for
certain plate combinations were recalculated. It was found that using this time period greater impulse
amelioration values were produced as the rate of pressure rise, dp/dt, was initially lower at the beginning
of the end wall pressure trace. Therefore, the lowest impulse amelioration value (7.9 %) achieved in this
study, would produce significant impulse amelioration (20.3 %) if it were to be used in a shelter’s
ventilation system. Impulse amelioration values were found to increase as the separation distance between
v
plates were increased. The average impulse amelioration value was found to increase approximately 1 %
for a 15mm increase in the distance between plates. The amplitude of the entire end wall pressure trace
was found to increase as the incident Mach number was increased. This resulted in greater initial peak
pressure and impulse experienced by the end wall. The significant attenuation of the incident shock wave
obtained during this study is attributed to the system of multiple reflected and transmitted waves that are
produced by the presence of the plate specimens in series. This increases the frequency of shock wave and
barrier interactions, when compared to just using a single barrier, creating regions of highly unsteady
flow, especially in the air space between the plate specimens. Furthermore, the presence of the series of
plates also allows for wave resonance to occur which may further attenuate the strength of the incident
shock wave. It is suggested that future studies include numerical techniques in order to further investigate
the complex wave processes that occur upon interaction with the plate specimens and confirm the major
loss mechanisms of the system.
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Experimental study of the hydrodynamics of high Mach number blast wavesEdens, Aaron Douglas 28 August 2008 (has links)
Not available / text
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Physics of three-dimensional normal shock wave/turbulent boundary layer interactions in rectangular channelsSami, Kashmir January 2012 (has links)
No description available.
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87 |
Fluid dynamics of the shock wave reactor /Masse, Robert K. January 2000 (has links)
Thesis (Ph. D.)--University of Washington, 2000. / Vita. Includes bibliographical references (p. 133-135).
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Near-steady oblique shock waves in a collisionless plasma / Lynn Mary OlsonOlson, Lynn Mary. January 1970 (has links)
Thesis (Ph. D.)--University of Wisconsin--Madison, 1970. / Vita. eContent provider-neutral record in process. Description based on print version record.
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Experimental study of the hydrodynamics of high Mach number blast wavesEdens, Aaron Douglas, Ditmire, Todd, January 2005 (has links) (PDF)
Thesis (Ph. D.)--University of Texas at Austin, 2005. / Supervisor: Todd Ditmire. Vita. Includes bibliographical references.
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Transducers for measuring acoustic transientsAlcock, Robin D. January 1997 (has links)
This thesis is concerned with the design and development of measuring devices for the characterisation of acoustic transients with high temporal and spatial resolution. Three new techniques are demonstrated characterising acoustic transients generated by Nd-YAG laser (1060nm, 30ns, 55mJ) assisted breakdown of water and air. The first technique demonstrates the use of a high power semiconductor laser in a high speed multiple exposure imaging system. This system developed is capable of illuminating an event with up to 10 pulses of light at a maximum repetition rate of 5MHz, with a timing accuracy of ≈5ns. Each semiconductor laser light pulse has a FWHM duration of 50ns, peak power of 30W, and a wavelength of 860nm. Images of individual acoustic transients are displayed on the same CCD camera frame, and it was found that this is best achieved using a dark field imaging technique such as Schlieren imaging.
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