TY - JOUR
T1 - Measurements of surface thermal structure, kinematics, and turbulence of a large-scale solitary breaking wave using infrared imaging techniques
AU - Huang, Zhi Cheng
AU - Hwang, Kao Shu
N1 - Funding Information:
We sincerely thank Luc Lenain and Prof. W. Kendall Melville for their assistance and support. Prof. Herchang Ay is thanked for providing the infrared camera. We thank Prof. H. H. Hwung and the staffs at the Tainan Hydraulics Laboratory and the Marine Physical Laboratory, Scripps Institution of Oceanography, UCSD, for offering the facilities and conducting the experiments. The anonymous reviewers are acknowledged for their valuable comments and suggestions. We thank the Taiwan Ministry of Science and Technology , International Wave Dynamics Research Center , National Cheng Kung University , for financial support (grant nos. MOST 103-2611-M-008-003 , NSC 101-2611-M-008-002 , NSC 103-2911-I-006-302 , and NSC 97-2221-E-006-259-MY3 ). This research was, in part, supported by the Ministry of Education, Taiwan (R.O.C.) under project: The Aim for the Top University Project to the NCKU. We also thank Prof. Phillips L.-F. Liu for his fruitful discussions.
Publisher Copyright:
© 2014 Elsevier B.V.
PY - 2015/2/1
Y1 - 2015/2/1
N2 - The surface temperature fields of large-scale solitary breaking waves are measured using infrared imaging techniques in a laboratory surf and swash zone. The surface velocity fields obtained by cross-correlating the images are decomposed into wave and turbulent motions using two filtering methods in the spatial and temporal domains. The techniques presented here provide new quantitative descriptions for the evolution of the surface thermal structures, kinematics, and turbulence that are induced by unsteady and highly foamy turbulent coastal flows. Novel organized streaks of thermal structures, which exhibit a finger-like shape, are found on the water surface of the crest roller behind the head of the rebounding jet. These thermal streaks evolve with time and become isotropic when returning to the surrounding bulk water temperature. The Froude-scaled maximum flow speed, accelerations, and vorticity are O(1), and the scaled turbulent kinetic energy (TKE) is O(-. 1); these results are similar to previous findings from numerical results and periodic surf-zone breakers. Significant and concentrated structures of these quantities occur in the moving wave crest during the uprush phase; however, these structures only develop during the late stages of the backwash phase. The TKE increases shoreward from the surf to the swash zones. The ratio of the averaged variance of the turbulent velocity in the wave breaking zone does not agree with the canonical prediction for plane-wake turbulence; however, the ratio is similar to that of boundary-layer turbulence and decreases in the bore region and the swash zone, indicating an increase in the turbulence anisotropy shoreward from the surf to the shallower swash flow.
AB - The surface temperature fields of large-scale solitary breaking waves are measured using infrared imaging techniques in a laboratory surf and swash zone. The surface velocity fields obtained by cross-correlating the images are decomposed into wave and turbulent motions using two filtering methods in the spatial and temporal domains. The techniques presented here provide new quantitative descriptions for the evolution of the surface thermal structures, kinematics, and turbulence that are induced by unsteady and highly foamy turbulent coastal flows. Novel organized streaks of thermal structures, which exhibit a finger-like shape, are found on the water surface of the crest roller behind the head of the rebounding jet. These thermal streaks evolve with time and become isotropic when returning to the surrounding bulk water temperature. The Froude-scaled maximum flow speed, accelerations, and vorticity are O(1), and the scaled turbulent kinetic energy (TKE) is O(-. 1); these results are similar to previous findings from numerical results and periodic surf-zone breakers. Significant and concentrated structures of these quantities occur in the moving wave crest during the uprush phase; however, these structures only develop during the late stages of the backwash phase. The TKE increases shoreward from the surf to the swash zones. The ratio of the averaged variance of the turbulent velocity in the wave breaking zone does not agree with the canonical prediction for plane-wake turbulence; however, the ratio is similar to that of boundary-layer turbulence and decreases in the bore region and the swash zone, indicating an increase in the turbulence anisotropy shoreward from the surf to the shallower swash flow.
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U2 - 10.1016/j.coastaleng.2014.12.005
DO - 10.1016/j.coastaleng.2014.12.005
M3 - Article
AN - SCOPUS:84920941507
SN - 0378-3839
VL - 96
SP - 132
EP - 147
JO - Coastal Engineering
JF - Coastal Engineering
ER -