FLOW IN THE NEIGHBORHOOD OF THE BREAKPOINT OF THE LEADING EDGE THIN WING AT THE STRONG INTERACTION REGIME

2011 ◽  
Vol 42 (2) ◽  
pp. 151-167 ◽  
Author(s):  
A. V. Ledovskiy ◽  
G. N. Dudin
2003 ◽  
Vol 18 (supp01) ◽  
pp. 1-26
Author(s):  
Richard Kenway

In the Standard Model, quarks and gluons are permanently confined by the strong interaction into hadronic bound states. The values of the quark masses and the strengths of the decays of one quark flavour into another cannot be measured directly, but must be deduced from experiments on hadrons. This requires calculations of the strong-interaction effects within the bound states, which are only possible using numerical simulations of lattice QCD. These are computationally intensive and, for the past twenty years, have exploited leading-edge computing technology. In conjunction with experimental data from B Factories, over the next few years, lattice QCD may provide clues to physics beyond the Standard Model. These lectures provide a non-technical introduction to lattice QCD, some of the recent results, QCD computers, and the future prospects.


2019 ◽  
Vol 487 (1) ◽  
pp. 24-27
Author(s):  
G. N. Dudin ◽  
V. Ya. Neyland

The flow around the yawed plate in the regime of strong interaction is considered in the case when the pressure at its trailing edge is not constant, but changes along the transverse coordinate. It is shown that in the case of large transverse gradients of the induced pressure, the type of expansions of flow functions in the vicinity of the leading edge changes significantly and the third term of the expansions should be taken into account.


1999 ◽  
Vol 32 (3) ◽  
pp. 631-647 ◽  
Author(s):  
L Adoui ◽  
C Caraby ◽  
A Cassimi ◽  
D Lelièvre ◽  
J P Grandin ◽  
...  

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