Measurements of surface thermal structure, kinematics, and turbulence of a large-scale solitary breaking wave using infrared imaging techniques

被引:16
作者
Huang, Zhi-Cheng [1 ]
Hwang, Kao-Shu [2 ,3 ]
机构
[1] Natl Cent Univ, Grad Inst Hydrol & Ocean Sci, Taoyuan 320, Taiwan
[2] Tainan Hydraul Lab, Tainan 709, Taiwan
[3] Natl Cheng Kung Univ, Int Wave Dynam Res Ctr, Tainan 701, Taiwan
关键词
Infrared; Solitary wave; Wave breaking; Swash zone; Turbulence; DOPPLER-VELOCIMETER DATA; SWASH-ZONE; RUN-UP; LABORATORY OBSERVATIONS; SEDIMENT SUSPENSION; WATER; FIELD; HYDRODYNAMICS; EVOLUTION; FLOW;
D O I
10.1016/j.coastaleng.2014.12.005
中图分类号
TU [建筑科学];
学科分类号
0813 ;
摘要
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. (C) 2014 Elsevier B.V. All rights reserved.
引用
收藏
页码:132 / 147
页数:16
相关论文
共 68 条
[1]   Sediment suspension and turbulence in the swash zone of dissipative beaches [J].
Aagaard, T ;
Hughes, MG .
MARINE GEOLOGY, 2006, 228 (1-4) :117-135
[2]   Kinematics of breaking tsunami wavefronts: A data set from large scale laboratory experiments [J].
Baldock, T. E. ;
Cox, D. ;
Maddux, T. ;
Killian, J. ;
Fayler, L. .
COASTAL ENGINEERING, 2009, 56 (5-6) :506-516
[3]   SURF-ZONE DYNAMICS [J].
BATTJES, JA .
ANNUAL REVIEW OF FLUID MECHANICS, 1988, 20 :257-293
[4]   Experimental investigation of turbulence generated by breaking waves in water of intermediate depth [J].
Chang, KA ;
Liu, PLF .
PHYSICS OF FLUIDS, 1999, 11 (11) :3390-3400
[5]   Vertical variation of the flow across the surf zone [J].
Christensen, ED ;
Walstra, DJ ;
Emerat, N .
COASTAL ENGINEERING, 2002, 45 (3-4) :169-198
[6]   Experimental study on the hydrodynamics of regular breaking waves [J].
De Serio, F ;
Mossa, M .
COASTAL ENGINEERING, 2006, 53 (01) :99-113
[7]   Hydrodynamics and sediment transport in the swash zone: a review and perspectives [J].
Elfrink, B ;
Baldock, T .
COASTAL ENGINEERING, 2002, 45 (3-4) :149-167
[8]   Quality control of acoustic Doppler velocimeter data in the surfzone [J].
Elgar, S ;
Raubenheimer, B ;
Guza, RT .
MEASUREMENT SCIENCE AND TECHNOLOGY, 2005, 16 (10) :1889-1893
[9]   Observations of the Surf-Zone Turbulent Dissipation Rate [J].
Feddersen, Falk .
JOURNAL OF PHYSICAL OCEANOGRAPHY, 2012, 42 (03) :386-399
[10]   Quality Controlling Surf Zone Acoustic Doppler Velocimeter Observations to Estimate the Turbulent Dissipation Rate [J].
Feddersen, Falk .
JOURNAL OF ATMOSPHERIC AND OCEANIC TECHNOLOGY, 2010, 27 (12) :2039-2055