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Coupled Atmospheric and Oceanic Effects on Mixed Layer Depth Variability

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... Lag. Internal wave Experiment. ITEX1 (Apr 94) Phase Lag ... Kraus, E.B. and J.S. Turner. A dynamic thermodynamic sea ice model. Tellus, 19, 98-105, 1967. ... – PowerPoint PPT presentation

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Title: Coupled Atmospheric and Oceanic Effects on Mixed Layer Depth Variability


1
Coupled Atmospheric and Oceanic Effects on Mixed
Layer Depth Variability
  • Operational Oceanography
  • OC/MR3570
  • William Swick

2
Project Goals
  • To further understanding of the role of air-sea
    influences on the oceanic mixed layer.
  • Navy Impacts
  • USW
  • Sound Velocity Profile

3
Description of Data
  • Station S2 (PC Tides Model Run and CTD Timeseries
    Location
  • Rain Gauge Stations
  • Conductivity, temperature and depth (CTD)
  • 29 hr timeseries (02 03 Feb)
  • UDAS
  • Wind Speed
  • Air Temp
  • Humidity
  • Solar Radiation
  • Sea Surface Temperature
  • PC Tides
  • 0900L 02 Feb - 1400L 03 Feb
  • Rain Gauge
  • Six Stations

4
Coupled Atmosphere-Ocean Effects
  • Surface stress provided by wind forcing
  • Buoyancy forcing related to the thermal exchanges
    between atmosphere and ocean
  • Salinity Fluxes related to precipitation and
    evaporation.
  • Vertical motion at the Mixed Layer Depth (-h)
  • Internal Waves

5
(No Transcript)
6
Ocean
  • Large Contributor to Variability
  • Amplitude increases with depth
  • Internal Wave 20m Amplitude
  • Tidally Forced Internal Wave
  • Phase Lag
  • Internal wave Experiment
  • ITEX1 (Apr 94)

7
Are the atmospheric effects negligible compared
to such a significant internal wave???
8
Atmospheric Effects
  • Heating
  • Qo () cooling
  • Qo (-) heating
  • Wind
  • Rain

9
Entrainment
  • we () means mixing of water from below deeping
    the mixed layer
  • we (-) is not physical. Water cannot be unmixed

10
Tale of two regimes
  • Deepening regime
  • Only positive or zero
  • Krauss and Turner Mixed Layer Depth Equation only
    holds for deepening regimes.
  • Atm-Ocean coupling
  • Salinity and Temperature Jumps
  • As h decreases. Entrainment increases
  • Shallowing Regime
  • How it works physically

11
.04
.07
Negative effect
Positive effect
Which is dominant?
Salinity dominates Temperature
12
  • Mixed Layer is shallowing due to
    precipitation!!!
  • Atmospheric conditions predict the mixed layer
    depth

13
Shallowing Regime
Using ships winds, calculated cooling rate, and
observed mixed layer depth we can calculate the
estimated rain rate.
14
Rain rate comparision
  • Wind 5 m/s
  • Cooling rate 25 W/m/m
  • Observed mixed layer depth 16m
  • Calculated rain rate per hour 0.37 cm/hr

15
Is that the answer?
  • Dynamic Problem
  • Advection/River Input
  • Function of (Wind, Total Surface Heat Flux, Mixed
    Layer Depth)
  • Rain rate variability
  • Spatial/Temporal
  • What happened after 1900L?

16
  • Precipitation rate has slowed allowing
    entrainment.
  • Mixed Layer is in a deepening regime
  • Ocean inputs provide for a rapid Mixed Layer
    Deepening

17
Conclusion
  • Mixed Layer Depth Variability
  • Two Regimes
  • Shallowing
  • Atmospheric Inputs determine shallowing
  • Underlying Ocean T-S profile is not felt
  • Vertical Motion at h is still important
  • Deepening
  • Atm-Ocean are strongly coupled
  • Highly variable
  • Atm (Wind/Heat/Rain)
  • Ocean (Salinity and Temperature Jumps, Vertical
    Motion at h)
  • In a deepening regime, we(), in an area like
    Monterey Bay (large internal waves) the vertical
    motion will tend to dominant.
  • During a shallowing regime the atmospheric inputs
    determine mixed layer depth along with the
    internal wave component.

18
Questions?
19
References
  • Garwood, R.W., Jr. An oceanic mixed layer model
    capable of simulating cyclic states. J. Phys.
    Oceanogr., 7, 455-471, 1977.
  • Garwood, R.W., Jr. Enhancements to deep turbulent
    entrainment. In Deep Convection and Deep Water
    Formation in the Ocean, Ed. by P. C. Chu and J.
    C. Gascard, Elsevier, 189-205, 1991.
  • Kraus, E.B. and J.S. Turner. A dynamic
    thermodynamic sea ice model. Tellus, 19, 98-105,
    1967.
  • Rosenfeld, L.K., J.D. Paduan, E.T. Petruncio, and
    J.E. Goncalves, 1999 Numerical simulations and
    observations of the internal tide in a submarine
    canyon. Proceedings, 'Aha Huliko'a Hawaiian
    Winter Workshop, University of Hawaii at Manoa,
    January 19-22.
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