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Multiscale preferential sweeping of particles settling in turbulence – CORRIGENDUM

Published online by Cambridge University Press:  14 June 2019

Josin Tom and
Andrew D. Bragg
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Abstract

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Information

Type
Corrigendum
Information
Journal of Fluid Mechanics , Volume 872 , 10 August 2019, pp. 995
Copyright
© 2019 Cambridge University Press 

In Tom & Bragg (Reference Tom and Bragg2019) the ordinate axis label of figure 5 was incorrect. The correct version of this figure is shown below.

Figure 5.

DNS results for $\langle u_{z}^{\prime }(\boldsymbol{x}^{p}(t),t)\rangle /u_{\unicode[STIX]{x1D702}}$ as a function of $St$ , for $Fr=0.052$ , and for various filtering lengths $\ell _{F}/\unicode[STIX]{x1D702}$ . The circles correspond to $R_{\unicode[STIX]{x1D706}}=90$ , the triangles to $R_{\unicode[STIX]{x1D706}}\approx 230$ and the squares to $R_{\unicode[STIX]{x1D706}}=398$ . The solid lines correspond to $\ell _{F}/\unicode[STIX]{x1D702}=\infty$ , the dashed lines to $\ell _{F}/\unicode[STIX]{x1D702}=125.6$ , the dash-dot lines to $\ell _{F}/\unicode[STIX]{x1D702}=31.4$ , and the dotted lines to $\ell _{F}/\unicode[STIX]{x1D702}=12.6$ .

References

Tom, J. & Bragg, A. D. 2019 Multiscale preferential sweeping of particles settling in turbulence. J. Fluid Mech. 871, 244–270.Google Scholar
Figure 0

Figure 5.DNS results for $\langle u_{z}^{\prime }(\boldsymbol{x}^{p}(t),t)\rangle /u_{\unicode[STIX]{x1D702}}$ as a function of $St$, for $Fr=0.052$, and for various filtering lengths $\ell _{F}/\unicode[STIX]{x1D702}$. The circles correspond to $R_{\unicode[STIX]{x1D706}}=90$, the triangles to $R_{\unicode[STIX]{x1D706}}\approx 230$ and the squares to $R_{\unicode[STIX]{x1D706}}=398$. The solid lines correspond to $\ell _{F}/\unicode[STIX]{x1D702}=\infty$, the dashed lines to $\ell _{F}/\unicode[STIX]{x1D702}=125.6$, the dash-dot lines to $\ell _{F}/\unicode[STIX]{x1D702}=31.4$, and the dotted lines to $\ell _{F}/\unicode[STIX]{x1D702}=12.6$.