Seasonal variability of thermocline in the Yellow Sea

来源 :Chinese Journal of Oceanology and Limnology | 被引量 : 0次 | 上传用户:sun_sun
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Based on the MASNUM wave-tide-circulation coupled numerical model, seasonal variability of thermocline in the Yellow Sea was simulated and compared with in-situ observations. Both simulated mixed layer depth (MLD) and thermocline intensity have similar spatial patterns to the observations. The simulated maximum MLD are 8 m and 22 m, while the corresponding observed values are 13 m and 27 m in July and October, respectively. The simulated thermocline intensity are 1.2℃/m and 0.5℃/m in July and October, respectively, which are 0.6℃/m less than those of the observations. It may be the main reason why the simulated thermocline is weaker than the observations that the model vertical resolution is less precise than that of the CTD data which is 1 m. Contours of both simulated and observed thermocline intensity present a circle in general. The wave-induced mixing plays a key role in the formation of the upper mixed layer in spring and summer. Tidal mixing enhances the thermocline intensity. Buoyancy-driven m Based on the MASNUM wave-tide-time pass numerical model, seasonal variability of thermocline in the Yellow Sea was simulated and compared with in-situ observations. Both simulated mixed depth (MLD) and thermocline intensity have similar spatial patterns to the observations. The simulated maximum MLD are 8 m and 22 m, while the corresponding observed values ​​are 13 m and 27 m in July and October, respectively. The simulated thermocline intensity is 1.2 ° C / m and 0.5 ° C / m in July and October, respectively, which are be the main reason why the simulated thermocline is weaker than the observations that the model that vertical resolution is less precise than that of the CTD data which is 1 m. simulated and observed thermocline intensity present a circle in general. The wave-induced mixing plays a key role in the formation of the upper mixed layer in spring and summer. Tidal mixing enhances the the thermocline intens ity. Buoyancy-driven m
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