Density and flow structure in the Clyde Sea front

Research output: Contribution to journalArticlepeer-review

Standard Standard

Density and flow structure in the Clyde Sea front. / Rippeth, Tom; Kasai, Akihide; Simpson, John.
In: Continental Shelf Research, Vol. 19, No. 4, 01.11.1999, p. 1833-1848.

Research output: Contribution to journalArticlepeer-review

HarvardHarvard

Rippeth, T, Kasai, A & Simpson, J 1999, 'Density and flow structure in the Clyde Sea front', Continental Shelf Research, vol. 19, no. 4, pp. 1833-1848. https://doi.org/10.1016/S0278-4343(99)00042-4

APA

CBE

MLA

VancouverVancouver

Rippeth T, Kasai A, Simpson J. Density and flow structure in the Clyde Sea front. Continental Shelf Research. 1999 Nov 1;19(4):1833-1848. Epub 1999 Oct 18. doi: 10.1016/S0278-4343(99)00042-4

Author

Rippeth, Tom ; Kasai, Akihide ; Simpson, John. / Density and flow structure in the Clyde Sea front. In: Continental Shelf Research. 1999 ; Vol. 19, No. 4. pp. 1833-1848.

RIS

TY - JOUR

T1 - Density and flow structure in the Clyde Sea front

AU - Rippeth, Tom

AU - Kasai, Akihide

AU - Simpson, John

PY - 1999/11/1

Y1 - 1999/11/1

N2 - A well-defined front in temperature and salinity separates the stratified Clyde Sea water from the vertically well mixed water of the North Channel. The detailed structure of the front was observed in autumn 1990 by a combination of, repeated crossings of the front using a shipborne ADCP and a towed undulating CTD system, and the deployment of a fixed mooring system with temperature, salinity and velocity sensors for a period of 12 days. The results show that the front was situated on the Great Plateau near a contour of log(10)(H/U-2(3)) = 2.7 similar to 3.7 where H is the water depth and U-2 the amplitude of M-2 tidal velocity. The temperature structure in the Clyde Sea was inverted and the Clyde Sea surface temperature was lower than that of the vertically well mixed water in the North Channel. Since the salinity gradient was stronger than the temperature gradient with fresher water on the surface, the density structure was predominantly controlled by salinity. There were indications of warm and saline bottom water upwelling on the mixed side of the front during spring tides. This upwelling disappeared and the salinity and temperature structure at the front was more diffuse during the neap tide period. A jet-like along-front residual current was observed flowing to the northwest in the surface layer with a counter flow to the southeast in the bottom layer. The vertical difference in velocity was about 9 cm s(-1) and was approximately consistent with the shear determined from the thermal wind relation. Both cross- and along-front components of the current observed at the mooring station varied in response to the advection of the front, although both components had large variations with periods of less than one day and several days. The front was advected past the mooring system by a mean flow from the North Channel to the inner basin, while oscillating 3-5 km back and forth with the tidal currents. From the velocity at a current meter mooring and CTD data, the front was estimated to have moved up to 20 km during the observational period and the cross frontal velocity was inferred to be 3-4 cm s(-1)

AB - A well-defined front in temperature and salinity separates the stratified Clyde Sea water from the vertically well mixed water of the North Channel. The detailed structure of the front was observed in autumn 1990 by a combination of, repeated crossings of the front using a shipborne ADCP and a towed undulating CTD system, and the deployment of a fixed mooring system with temperature, salinity and velocity sensors for a period of 12 days. The results show that the front was situated on the Great Plateau near a contour of log(10)(H/U-2(3)) = 2.7 similar to 3.7 where H is the water depth and U-2 the amplitude of M-2 tidal velocity. The temperature structure in the Clyde Sea was inverted and the Clyde Sea surface temperature was lower than that of the vertically well mixed water in the North Channel. Since the salinity gradient was stronger than the temperature gradient with fresher water on the surface, the density structure was predominantly controlled by salinity. There were indications of warm and saline bottom water upwelling on the mixed side of the front during spring tides. This upwelling disappeared and the salinity and temperature structure at the front was more diffuse during the neap tide period. A jet-like along-front residual current was observed flowing to the northwest in the surface layer with a counter flow to the southeast in the bottom layer. The vertical difference in velocity was about 9 cm s(-1) and was approximately consistent with the shear determined from the thermal wind relation. Both cross- and along-front components of the current observed at the mooring station varied in response to the advection of the front, although both components had large variations with periods of less than one day and several days. The front was advected past the mooring system by a mean flow from the North Channel to the inner basin, while oscillating 3-5 km back and forth with the tidal currents. From the velocity at a current meter mooring and CTD data, the front was estimated to have moved up to 20 km during the observational period and the cross frontal velocity was inferred to be 3-4 cm s(-1)

U2 - 10.1016/S0278-4343(99)00042-4

DO - 10.1016/S0278-4343(99)00042-4

M3 - Article

VL - 19

SP - 1833

EP - 1848

JO - Continental Shelf Research

JF - Continental Shelf Research

SN - 0278-4343

IS - 4

ER -