Simulations of Evaporating Spray Jet in a Uniform Co-Flowing Turbulent Air Stream

Numerical simulations are performed on the flow of fine, polydisperse droplets of acetone ejected from a round jet of air into an ambient turbulent, uniform co-flowing air stream. The objective is to validate the numerical model by comparing the predictions with experimental measurements of a well d...

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Main Authors: Santanu De, K.N. Lakshmisha
Format: Article
Language:English
Published: SAGE Publishing 2009-06-01
Series:International Journal of Spray and Combustion Dynamics
Online Access:https://doi.org/10.1260/175682709788707459
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spelling doaj-4a5c78ac0eb5495fa7f1db1908bc35502020-11-25T02:48:37ZengSAGE PublishingInternational Journal of Spray and Combustion Dynamics1756-82771756-82852009-06-01110.1260/17568270978870745910.1260_175682709788707459Simulations of Evaporating Spray Jet in a Uniform Co-Flowing Turbulent Air StreamSantanu DeK.N. LakshmishaNumerical simulations are performed on the flow of fine, polydisperse droplets of acetone ejected from a round jet of air into an ambient turbulent, uniform co-flowing air stream. The objective is to validate the numerical model by comparing the predictions with experimental measurements of a well defined evaporating spray configuration (Chen et al. , Int. J. Multiphase Flow 32(2006), 389–412). The carrier-phase is considered in the Eulerian context, while the dispersed phase is tracked in the Lagrangian framework. Various interactions between the two phases are taken into account by means of a two-way coupling. The stochastic separated flow (SSF) model is adopted for the spray calculations. The gas-phase turbulence terms are closed using the standard k -ε model. The spray evaporation is described using a thermal model with an infinite-conductivity. Overall, very good agreement is observed in the comparisons of the computational predictions and experimental measurements. The predicted droplet number-mean axial velocity, r.m.s. of fluctuating velocity for the various droplet classes at different downstream locations exhibit a self-similarity downstream of the nozzle exit. Near the nozzle-exit (around z/d jet = 5), the r.m.s. of droplet number mean axial fluctuating velocity attains a maximum within the shear layer near r/d jet = 0.4–0.6 for different droplet classes. Further downstream, the peak shifts towards the axis. A similar variation is noticed in the Sauter mean diameter (SMD) distribution of the droplets. It is concluded that, a higher level of turbulence leads to a faster depletion of the smaller droplets, resulting in an increase in the local droplet-SMD in those regions.https://doi.org/10.1260/175682709788707459
collection DOAJ
language English
format Article
sources DOAJ
author Santanu De
K.N. Lakshmisha
spellingShingle Santanu De
K.N. Lakshmisha
Simulations of Evaporating Spray Jet in a Uniform Co-Flowing Turbulent Air Stream
International Journal of Spray and Combustion Dynamics
author_facet Santanu De
K.N. Lakshmisha
author_sort Santanu De
title Simulations of Evaporating Spray Jet in a Uniform Co-Flowing Turbulent Air Stream
title_short Simulations of Evaporating Spray Jet in a Uniform Co-Flowing Turbulent Air Stream
title_full Simulations of Evaporating Spray Jet in a Uniform Co-Flowing Turbulent Air Stream
title_fullStr Simulations of Evaporating Spray Jet in a Uniform Co-Flowing Turbulent Air Stream
title_full_unstemmed Simulations of Evaporating Spray Jet in a Uniform Co-Flowing Turbulent Air Stream
title_sort simulations of evaporating spray jet in a uniform co-flowing turbulent air stream
publisher SAGE Publishing
series International Journal of Spray and Combustion Dynamics
issn 1756-8277
1756-8285
publishDate 2009-06-01
description Numerical simulations are performed on the flow of fine, polydisperse droplets of acetone ejected from a round jet of air into an ambient turbulent, uniform co-flowing air stream. The objective is to validate the numerical model by comparing the predictions with experimental measurements of a well defined evaporating spray configuration (Chen et al. , Int. J. Multiphase Flow 32(2006), 389–412). The carrier-phase is considered in the Eulerian context, while the dispersed phase is tracked in the Lagrangian framework. Various interactions between the two phases are taken into account by means of a two-way coupling. The stochastic separated flow (SSF) model is adopted for the spray calculations. The gas-phase turbulence terms are closed using the standard k -ε model. The spray evaporation is described using a thermal model with an infinite-conductivity. Overall, very good agreement is observed in the comparisons of the computational predictions and experimental measurements. The predicted droplet number-mean axial velocity, r.m.s. of fluctuating velocity for the various droplet classes at different downstream locations exhibit a self-similarity downstream of the nozzle exit. Near the nozzle-exit (around z/d jet = 5), the r.m.s. of droplet number mean axial fluctuating velocity attains a maximum within the shear layer near r/d jet = 0.4–0.6 for different droplet classes. Further downstream, the peak shifts towards the axis. A similar variation is noticed in the Sauter mean diameter (SMD) distribution of the droplets. It is concluded that, a higher level of turbulence leads to a faster depletion of the smaller droplets, resulting in an increase in the local droplet-SMD in those regions.
url https://doi.org/10.1260/175682709788707459
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