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The main purposes of this study are to generate a large turbulence scale and simulate a turbulent flow fitted to specified power spectrum and co-coherence in a low frequency range, both of which are not easily accomplished only by the means of roughness blocks, spires and grids.
Finally, large turbulence intensity is generated in the plane of wind turbine rotation.
It was relatively easy to obtain a large turbulence scale by controlling multiple fans numerically.
The second sound field is generated in a similar manner involving the large turbulence structures and the shock cells in the inner shear layer of the jet.
This formula is more effective for evaluating thermal comfort in the outdoor environment where there is large turbulence, because conventional formulae can evaluate only the influences of velocity.
It is believed that one of the observed noise sources is the large turbulence structures of the jet flow and the other observed noise source is the fine scale turbulence.
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Two grids are used — one is a standard biplanar grid, while the second is a new design that provides larger turbulence length scales.
The differences are illuminating: the continuous-adjoint is shown to suffer from exponential error growth in (reverse) time even for the best-resolved largest turbulence scales.
Matoza et al. (2009) contended that sustained eruption noise has its source in large scale turbulence, favouring a quadrupole source.
In these circumstances the ability to obtain a large enough turbulence integral scale is usually compromised by the limited dimensions of the wind tunnel.
We validate the LBM at Reynolds numbers beyond the limit of Darcy's law, and compare the results of direct numerical simulation with those achieved by applying a Smagorinsky-type large eddy turbulence model.
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