TY - JOUR
T1 - Effects of varying pycnocline thickness on interfacial wave generation and propagation
AU - Cheng, M.
AU - Hsu, John
PY - 2014
Y1 - 2014
N2 - Interfacial solitary waves (ISWs) can be observed in stratified ocean and laboratory flumes which generally comprise a pycnocline in finite thickness. This has led to the adoption of a two-layer or three-layer fluid system for studying the ISWs. However, this assumption has limited success for understanding the effects of variable pycnocline thicknesses on the wave generation and propagation. This paper discusses the broadening of pycnocline thickness on the generation of an ISW in a wave flume and its subsequent effects on wave amplitude and potential energy across a submerged trapezoidal obstacle under laboratory conditions. Three different definitions for the nominal pycnocline thickness are discussed, based on the measured fluid density profiles and the calculated buoyant frequency profiles. As the pycnocline thickness increased after repeated wave-makings, the incident ISW amplitude decreased as expected, as well as the wave speed across the obstacle. Moreover, as the thickness broadened, the fluid system appeared to contain two or multiple peaks rather than single peak when the pycnocline was thin and finite. This implies that the resultant wave might consist of several modes (at least mode-2) in the flume even at its generation stage. © 2014 Elsevier Ltd.
AB - Interfacial solitary waves (ISWs) can be observed in stratified ocean and laboratory flumes which generally comprise a pycnocline in finite thickness. This has led to the adoption of a two-layer or three-layer fluid system for studying the ISWs. However, this assumption has limited success for understanding the effects of variable pycnocline thicknesses on the wave generation and propagation. This paper discusses the broadening of pycnocline thickness on the generation of an ISW in a wave flume and its subsequent effects on wave amplitude and potential energy across a submerged trapezoidal obstacle under laboratory conditions. Three different definitions for the nominal pycnocline thickness are discussed, based on the measured fluid density profiles and the calculated buoyant frequency profiles. As the pycnocline thickness increased after repeated wave-makings, the incident ISW amplitude decreased as expected, as well as the wave speed across the obstacle. Moreover, as the thickness broadened, the fluid system appeared to contain two or multiple peaks rather than single peak when the pycnocline was thin and finite. This implies that the resultant wave might consist of several modes (at least mode-2) in the flume even at its generation stage. © 2014 Elsevier Ltd.
U2 - 10.1016/j.oceaneng.2014.05.018
DO - 10.1016/j.oceaneng.2014.05.018
M3 - Article
SN - 0029-8018
VL - 88
SP - 34
EP - 45
JO - Ocean Engineering
JF - Ocean Engineering
ER -