TY - JOUR
T1 - A benchmark for particle-laden turbulent duct flow
T2 - A joint computational and experimental study
AU - Esmaily, M.
AU - Villafane, L.
AU - Banko, A. J.
AU - Iaccarino, G.
AU - Eaton, J. K.
AU - Mani, A.
N1 - Funding Information:
This work was funded by the United States Department of Energy’s (DoE) National Nuclear Security Administration (NNSA) under the Predictive Science Academic Alliance Program II (PSAAP II) at Stanford University.
Publisher Copyright:
© 2020
PY - 2020/11
Y1 - 2020/11
N2 - A turbulent duct flow laden with small heavy inertial particles (Reτ ≈ 570, St+≈50, dp+≈0.3, St ≈ 12, and dp/η ≈ 0.17) is studied computationally and experimentally. We examine whether a long development section can be modeled using a short periodic domain. This simplification is not valid if the development section is too short (less than 25–50 duct-height in our case), the periodic simulation is not integrated long enough (less than O(1000) large-eddy turnover time in our case), or the effective mass loading ratio is not adjusted correctly (increased by a factor of 1.5 in our case). Additionally, we show that ignoring particle-particle collisions, even when the volume fraction is as low as 3.9×10−6, produces a large over-estimation of near-wall particle concentration (turbophoresis). The necessity of tailored post-processing of simulations for a one-to-one comparison against experiments is demonstrated. Namely, the finite thickness of the laser sheet and the optically-sampled volume size should be considered when post-processing simulations to reproduce the experimental measurement of clustering statistics. Experimentally and computationally, we show that an increase in the mass-loading ratio from 2.4% to 12% has a minimal effect on clustering, slightly lowers velocity fluctuations, and diminishes turbophoresis.
AB - A turbulent duct flow laden with small heavy inertial particles (Reτ ≈ 570, St+≈50, dp+≈0.3, St ≈ 12, and dp/η ≈ 0.17) is studied computationally and experimentally. We examine whether a long development section can be modeled using a short periodic domain. This simplification is not valid if the development section is too short (less than 25–50 duct-height in our case), the periodic simulation is not integrated long enough (less than O(1000) large-eddy turnover time in our case), or the effective mass loading ratio is not adjusted correctly (increased by a factor of 1.5 in our case). Additionally, we show that ignoring particle-particle collisions, even when the volume fraction is as low as 3.9×10−6, produces a large over-estimation of near-wall particle concentration (turbophoresis). The necessity of tailored post-processing of simulations for a one-to-one comparison against experiments is demonstrated. Namely, the finite thickness of the laser sheet and the optically-sampled volume size should be considered when post-processing simulations to reproduce the experimental measurement of clustering statistics. Experimentally and computationally, we show that an increase in the mass-loading ratio from 2.4% to 12% has a minimal effect on clustering, slightly lowers velocity fluctuations, and diminishes turbophoresis.
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U2 - 10.1016/j.ijmultiphaseflow.2020.103410
DO - 10.1016/j.ijmultiphaseflow.2020.103410
M3 - Article
AN - SCOPUS:85089386734
SN - 0301-9322
VL - 132
JO - International Journal of Multiphase Flow
JF - International Journal of Multiphase Flow
M1 - 103410
ER -