Experimental study on sand bed excavation by impinging swirling jets

2011 ◽  
Vol 49 (5) ◽  
pp. 601-610 ◽  
Author(s):  
Joaquin Ortega-Casanova ◽  
Nicolas Campos ◽  
Ramon Fernandez-Feria
1989 ◽  
Author(s):  
M. NIKJOOY ◽  
H. MONGIA ◽  
G. SAMUELSEN ◽  
V. MCDONELL

2018 ◽  
Vol 12 (6) ◽  
pp. 533
Author(s):  
Andreas Naxakis ◽  
Konstantinos Perrakis ◽  
Thrassos Panidis

2009 ◽  
Author(s):  
J. Naughton ◽  
D. Stanescu ◽  
S. Heinz ◽  
R. Semaan ◽  
M. Stoellinger ◽  
...  

AIAA Journal ◽  
2008 ◽  
Vol 46 (8) ◽  
pp. 2002-2009 ◽  
Author(s):  
Abolfazl Shiri ◽  
William K. George ◽  
Jonathan W. Naughton

2021 ◽  
Vol 2119 (1) ◽  
pp. 012023
Author(s):  
A S Nebuchinov

Abstract The aim of this work is to study the effect of different forms of passive change in the shape of the flow on the intensity of heat transfer in the impact jet. In this work, a cycle of experiments was performed to investigate an axisymmetric jet flowing normally onto a heated surface. The jet was located both in natural conditions and during swirling of the flow (S = 0.4; 0.7; 1.0). It is shown that the intensity of heat transfer on a heated target in the case of a chevrons jet has little effect on the character, but significantly intensifies heat transfer. In the case of a swirling jet, the intensity distribution on the wall changes its character and locally increases at small distances between the nozzle and the heater.


Author(s):  
Norio Baba ◽  
Norihiko Ichise ◽  
Syunya Watanabe

The tilted beam illumination method is used to improve the resolution comparing with the axial illumination mode. Using this advantage, a restoration method of several tilted beam images covering the full azimuthal range was proposed by Saxton, and experimentally examined. To make this technique more reliable it seems that some practical problems still remain. In this report the restoration was attempted and the problems were considered. In our study, four problems were pointed out for the experiment of the restoration. (1) Accurate beam tilt adjustment to fit the incident beam to the coma-free axis for the symmetrical beam tilting over the full azimuthal range. (2) Accurate measurements of the optical parameters which are necessary to design the restoration filter. Even if the spherical aberration coefficient Cs is known with accuracy and the axial astigmatism is sufficiently compensated, at least the defocus value must be measured. (3) Accurate alignment of the tilt-azimuth series images.


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