scholarly journals Direct Numerical Simulations of Grouping Effects in Droplet Streams Using Different Boundary Conditions

2021 ◽  
Vol 1 (1) ◽  
Author(s):  
Matthias Ibach ◽  
Kathrin Schulte ◽  
Visakh Vaikuntanathan ◽  
Alumah Arad ◽  
David Katoshevski ◽  
...  
2012 ◽  
Vol 528 ◽  
pp. 119-126
Author(s):  
T. Korepanova ◽  
V.P. Matveenko ◽  
N. Sevodina

Numerical method is proposed for construction of singular solutions for spatial crossing wedge-and cone-shaped cracks. The results of numerical simulations made in the study allowed us to estimate the stress singularity indices at the tip of wedge-shaped cracks for different boundary conditions on the crack faces and at the tip of crossing cone cracks. The stress singularity at the tips of cone-shaped cracks is investigated.


2010 ◽  
Vol 6 (S271) ◽  
pp. 403-404
Author(s):  
Regner Trampedach ◽  
Kyle Augustson

AbstractDirect numerical simulations of convective stellar envelopes, are divided between two different physical regimes, that are rather difficult to reconcile — at least with the computational power of present-day computers. This paper outlines an attempt at bridging the gap between surface and interior simulations of convection.


2011 ◽  
Vol 670 ◽  
pp. 581-605 ◽  
Author(s):  
GUILLERMO ARAYA ◽  
LUCIANO CASTILLO ◽  
CHARLES MENEVEAU ◽  
KENNETH JANSEN

A dynamic method for prescribing realistic inflow boundary conditions is presented for simulations of spatially developing turbulent boundary layers. The approach is based on the rescaling–recycling method proposed by Lund, Wu & Squires (J. Comput. Phys, vol. 140, 1998, pp. 233–258) and the multi-scale method developed by Araya, Jansen & Castillo (J. Turbul., vol. 10, no. 36, 2009, pp. 1–33). The rescaling process requires prior knowledge about how the velocity and length scales are related between the inlet and recycle stations. Here a dynamic approach is proposed in which such information is deduced dynamically by involving an additional plane, the so-called test plane located between the inlet and recycle stations. The approach distinguishes between the inner and outer regions of the boundary layer and enables the use of multiple velocity scales. This flexibility allows applications to boundary layer flows with pressure gradients and avoids the need to prescribe empirically the friction velocity and other flow parameters at the inlet of the domain. The dynamic method is tested in direct numerical simulations of zero, favourable and adverse pressure gradient flows. The dynamically obtained scaling exponents for the downstream evolution of boundary layer parameters are found to fluctuate in time, but on average they agree with the expected values for zero, favourable and adverse pressure gradient flows. Comparisons of the results with data from experiments, and from other direct numerical simulations that use much longer computational domains to capture laminar-to-turbulence transition, demonstrate the suitability of the proposed dynamic method.


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