Multiscale turbulence is a class of turbulent flows in which the chaotic motion of the fluid is forced at different length and/or time scales. This is usually achieved by immersing in a moving fluid a body with a multiscale, often fractal-like, arrangement of length scales. This arrangement of scales can be either passive or active
As turbulent flows contain eddies with a wide range of scales, exciting the turbulence at particular scales (or range of scales) allows one to fine-tune the properties of that flow. Multiscale turbulent flows have been successfully applied in different fields., such as:
Reducing acoustic noise from wings by modifying the geometry of spoilers; Enhancing heat transfer from impinging jets passing through grids; Reducing the vortex shedding intensity of flows past normal plates without changing the shedding frequency; Enhancing mixing by energy-efficient stirring; Improving flow metering and flow conditioning in pipes; Improving combustion.
Multiscale turbulence has also played an important role into probing the internal structure of turbulence. This sort of turbulence allowed researchers to unveil a novel dissipation law in which the parameter C ϵ {\displaystyle C_{\epsilon }} in
ε = C ε U 3 L {\displaystyle \varepsilon =C_{\varepsilon }{\frac {{\mathcal {U}}^{3}}{\mathcal {L}}}}
is not constant, as required by the Richardson-Kolmogorov energy cascade. This new law can be expressed as C ϵ ∝ R e I m R e L n {\displaystyle C_{\epsilon }\propto {\frac {Re_{I}^{m}}{Re_{L}^{n}}}} , with m ≈ 1 ≈ n {\displaystyle m\approx 1\approx n} , where R e I {\displaystyle Re_{I}} and R e L {\displaystyle Re_{L}} are Reynolds numbers based, respectively, on initial/global conditions (such as free-stream velocity and the object's length scale) and local conditions (such as the rms velocity and integral length scale). This new dissipation law characterises non-equilibrium turbulence apparently universally in various flows (not just multiscale turbulence) and results from non-equilibrium unsteady energy cascade. This imbalance implies that new mean flow scalings exist for free shear turbulent flows, as already observed in axisymmetric wakes
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