Numerical investigation of secondary peaks in Nusselt profile under water jet impingement
In the present work, numerical simulations were conducted to observe the occurrence of secondary peaks in Nusselt profiles, which were generated on the target surface due to the impingement of water. Simulations were carried out in an ANSYS CFX solver by varying the Reynolds number Re from 825 to...
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American Institute of Aeronautics and Astronautics
2020
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在線閱讀: | http://irep.iium.edu.my/80218/7/80218%20Numerical%20investigation%20of%20secondary%20peaks.pdf http://irep.iium.edu.my/80218/13/80218_Numerical%20investigation%20of%20secondary%20peaks_SCOPUS.pdf http://irep.iium.edu.my/80218/ https://arc.aiaa.org/doi/abs/10.2514/1.T5905 |
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my.iium.irep.802182021-01-18T02:04:29Z http://irep.iium.edu.my/80218/ Numerical investigation of secondary peaks in Nusselt profile under water jet impingement Siddiqui, Umair Ansari, Emad Khan, Sher Afghan Patil, Rajesh TJ Mechanical engineering and machinery In the present work, numerical simulations were conducted to observe the occurrence of secondary peaks in Nusselt profiles, which were generated on the target surface due to the impingement of water. Simulations were carried out in an ANSYS CFX solver by varying the Reynolds number Re from 825 to 41,292 and the nozzle-target spacing (Z∕d) from 0.25 to 4. A k-ε turbulence model with realizable equations having an optimum grid size (minimum face size of 0.0008575 and number of elements of 1,225,616) was incorporated. This computational domain with the mentioned grid size was subjected to various boundary conditions (for plotting the Nusselt profile for different impinging and geometric parameters). It was found that the high velocities of jets with lower nozzle-target spacings were the leading causes for the occurrence of secondary peaks in the Nusselt profile. A nondimensional constant was defined as the ratio of the Reynolds number to the nozzle-target spacing, carrying a threshold magnitude above which secondary peaks in Nusselt profiles were bound to happen. The value of this nondimensional constant �Re∕�Z∕d�� was approximated to 1000. The occurrence of an intermediate transition region due to the imbalance penetrating momentum was the true cause of the occurrence of secondary peaks. This was justified using velocity contours. American Institute of Aeronautics and Astronautics 2020-04-25 Article PeerReviewed application/pdf en http://irep.iium.edu.my/80218/7/80218%20Numerical%20investigation%20of%20secondary%20peaks.pdf application/pdf en http://irep.iium.edu.my/80218/13/80218_Numerical%20investigation%20of%20secondary%20peaks_SCOPUS.pdf Siddiqui, Umair and Ansari, Emad and Khan, Sher Afghan and Patil, Rajesh (2020) Numerical investigation of secondary peaks in Nusselt profile under water jet impingement. Journal of Thermophysics and Heat Transfer, 34 (2 (April-June)). pp. 421-428. ISSN 0887-8722 E-ISSN 1533-6808 https://arc.aiaa.org/doi/abs/10.2514/1.T5905 |
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TJ Mechanical engineering and machinery Siddiqui, Umair Ansari, Emad Khan, Sher Afghan Patil, Rajesh Numerical investigation of secondary peaks in Nusselt profile under water jet impingement |
description |
In the present work, numerical simulations were conducted to observe the occurrence of secondary peaks in Nusselt
profiles, which were generated on the target surface due to the impingement of water. Simulations were carried out in
an ANSYS CFX solver by varying the Reynolds number Re from 825 to 41,292 and the nozzle-target spacing (Z∕d)
from 0.25 to 4. A k-ε turbulence model with realizable equations having an optimum grid size (minimum face size of 0.0008575 and number of elements of 1,225,616) was incorporated. This computational domain with the mentioned grid size was subjected to various boundary conditions (for plotting the Nusselt profile for different impinging and geometric parameters). It was found that the high velocities of jets with lower nozzle-target spacings were the leading causes for the occurrence of secondary peaks in the Nusselt profile. A nondimensional constant was defined as the ratio of the Reynolds number to the nozzle-target spacing, carrying a threshold magnitude above which secondary peaks in Nusselt profiles were bound to happen. The value of this nondimensional constant �Re∕�Z∕d�� was approximated to 1000. The occurrence of an intermediate transition region due to the imbalance penetrating momentum was the true cause of the occurrence of secondary peaks. This was justified using velocity contours. |
format |
Article |
author |
Siddiqui, Umair Ansari, Emad Khan, Sher Afghan Patil, Rajesh |
author_facet |
Siddiqui, Umair Ansari, Emad Khan, Sher Afghan Patil, Rajesh |
author_sort |
Siddiqui, Umair |
title |
Numerical investigation of secondary peaks in Nusselt profile under water jet impingement |
title_short |
Numerical investigation of secondary peaks in Nusselt profile under water jet impingement |
title_full |
Numerical investigation of secondary peaks in Nusselt profile under water jet impingement |
title_fullStr |
Numerical investigation of secondary peaks in Nusselt profile under water jet impingement |
title_full_unstemmed |
Numerical investigation of secondary peaks in Nusselt profile under water jet impingement |
title_sort |
numerical investigation of secondary peaks in nusselt profile under water jet impingement |
publisher |
American Institute of Aeronautics and Astronautics |
publishDate |
2020 |
url |
http://irep.iium.edu.my/80218/7/80218%20Numerical%20investigation%20of%20secondary%20peaks.pdf http://irep.iium.edu.my/80218/13/80218_Numerical%20investigation%20of%20secondary%20peaks_SCOPUS.pdf http://irep.iium.edu.my/80218/ https://arc.aiaa.org/doi/abs/10.2514/1.T5905 |
_version_ |
1690370716591980544 |
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13.250345 |