scholarly journals The Influence of the Computational Mesh on the Prediction of Vortex Interactions about a Generic Missile Airframe

2022 ◽  
Author(s):  
Erdem Dikbas ◽  
Christian Schnepf ◽  
Magnus H. Tormalm ◽  
Michael Anderson ◽  
Scott Shaw ◽  
...  
Author(s):  
Johan Roenby ◽  
Hassan Aref

The model of body–vortex interactions, where the fluid flow is planar, ideal and unbounded, and the vortex is a point vortex, is studied. The body may have a constant circulation around it. The governing equations for the general case of a freely moving body of arbitrary shape and mass density and an arbitrary number of point vortices are presented. The case of a body and a single vortex is then investigated numerically in detail. In this paper, the body is a homogeneous, elliptical cylinder. For large body–vortex separations, the system behaves much like a vortex pair regardless of body shape. The case of a circle is integrable. As the body is made slightly elliptic, a chaotic region grows from an unstable relative equilibrium of the circle-vortex case. The case of a cylindrical body of any shape moving in fluid otherwise at rest is also integrable. A second transition to chaos arises from the limit between rocking and tumbling motion of the body known in this case. In both instances, the chaos may be detected both in the body motion and in the vortex motion. The effect of increasing body mass at a fixed body shape is to damp the chaos.


AIAA Journal ◽  
2002 ◽  
Vol 40 (3) ◽  
pp. 474-480 ◽  
Author(s):  
Woo Seop Oh ◽  
Joo Sung Kim ◽  
Oh Joon Kwon

2013 ◽  
Vol 70 (3) ◽  
pp. 743-766 ◽  
Author(s):  
Akira Yamazaki ◽  
Hisanori Itoh

Abstract The selective absorption mechanism (SAM), newly proposed in Part I of this study on the maintenance mechanism of blocking, is verified through numerical experiments. The experiments were based on the nonlinear equivalent-barotropic potential vorticity equation, with varying conditions with respect to the shape and amplitude of blocking, and characteristics of storm tracks (displacement and strength) and background zonal flow. The experiments indicate that the SAM effectively maintains blocking, irrespective of the above conditions. At first, by applying a channel model on a β plane, numerical experiments were conducted using a uniform background westerly with and without a jet. The results show that the presence of a jet promotes the effectiveness of the SAM. Then, two types of spherical model experiments were also performed. In idealized experiments, the SAM was as effective as the β-plane model in explaining the maintenance of blocking. Moreover, experiments performed under realistic meteorological conditions showed that the SAM maintained a real block, demonstrating that the SAM is effective. These results, and the case study in Part I, verify that the SAM is the effective general maintenance mechanism for blocking.


2012 ◽  
Vol 2012 ◽  
pp. 1-15 ◽  
Author(s):  
Aldo Bonfiglioli ◽  
Renato Paciorri ◽  
Andrea Di Mascio

Within a continuum framework, flows featuring shock waves can be modelled by means of either shock capturing or shock fitting. Shock-capturing codes are algorithmically simple, but are plagued by a number of numerical troubles, particularly evident when shocks are strong and the grids unstructured. On the other hand, shock-fitting algorithms on structured grids allow to accurately compute solutions on coarse meshes, but tend to be algorithmically complex. We show how recent advances in computational mesh generation allow to relieve some of the difficulties encountered by shock capturing and contribute towards making shock fitting on unstructured meshes a versatile technique.


2001 ◽  
Vol T98 (1) ◽  
pp. 29 ◽  
Author(s):  
Jens Juul Rasmussen ◽  
Anders H. Nielsen ◽  
Volker Naulin

1997 ◽  
Author(s):  
Ashish Nedungadi ◽  
Mark Lewis ◽  
Ashish Nedungadi ◽  
Mark Lewis

2016 ◽  
Vol 29 (3) ◽  
pp. 035602 ◽  
Author(s):  
Qingyou Meng ◽  
Christopher N Varney ◽  
Hans Fangohr ◽  
Egor Babaev

1996 ◽  
Vol 113 (1) ◽  
pp. 429-449 ◽  
Author(s):  
S. K. AGGARWAL ◽  
T. W. PARK ◽  
V. R. KATTA

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