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The stagnation wall is oscillated sinusoidally along the stagnation streamline.
The oscillation of the stagnation wall induces the periodic fluctuations of flow velocity and flame stretch, and hence the fluctuations of flame displacement speed.
The amplitude of the flame stretch fluctuation increases with increasing frequency of the wall in the Strouhal number greater than unity owing to the increase in the amplitude of the oscillatory wall velocity, when the stagnation wall is oscillated along the stagnation streamline at constant amplitude.
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Only s = L = 0.5W (W = slot width) offered an excellent enhancement of heat transfer over that of the control (no plates) in the stagnation and wall-jet regions.
The potential of using a double-faced wall stagnation flow (DWSF) burner in mass production of multi-walled carbon nanotubes (MWCNTs) has been evaluated.
Microwave induced flame speed enhancement is quantified in a laminar, premixed CH4/air wall stagnation flat flame.
Flame-synthesis limits of carbon nanotubes (CNTs) are measured using a double-faced wall stagnation flow (DWSF) burner that shows potential in mass production of CNTs.
The experiment is performed using the jet-wall stagnation flame configuration and the particle imaging velocimetry (PIV) technique.
Experiments are carried out in the single jet-wall, stagnation flow configuration using laser Doppler velocimetry for the determination of the axial velocity profiles.
A flow can be stagnated by a solid wall or a free stagnation point or a line can exist in the interior of the fluid domain.
The results confirm that, for both flapper shapes, cavitation commonly occurs along the nozzle tip wall beyond stagnation region.
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