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Hypothesized Thermal Circulation Cell Associated with the Gulf Stream Andrew Condon Department of Marine and Environmental Systems Florida Institute of Technology Melbourne, FL 32901 July 15, 2004
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Overview Objectives What is a Thermal Circulation Cell? Ingredients of Cloud Formation Possible Gulf Stream Circulation Cell Data Collection Methods How do we know if it is there? / Results What influences its formation? Summary
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Objectives Why Objectives Why To determine whether or not a secondary thermal circulation cell due to the offshore sea surface temperature gradient associated with the Gulf Stream exists If it does exist how can it be identified and what strengthens and hinders its formation Not well documented, very little research conducted in this area Implications for Marine Meteorology / air-sea interaction Marine Interests (recreational and commercial): Clouds or thunderstorms along Gulf Stream
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Thermally-Forced Circulations Mesoscale (10’s-100’s km / hours) Differential Heating: Temperature Contrast Cooler more dense air causes higher pressure than warmer less dense air Pressure gradient exists and the wind starts to blow from high to low pressure
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Thermal Circulation Example: The Sea-Breeze Example: The Sea-Breeze
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Ingredients for Cloud Development Lift Convection (Thermals) Orographic Convergence Frontal Temperature Moisture
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Possible Gulf Stream Circulation Cell?
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Data Collection Methods Data Collected May 25, 26, and 27 2004 Visible Satellite Images from Global Hydrology and Climate Center Omega Cross Sections using GARP MODIS Satellite Images for the Gulf Stream Location RUC 850 mb Height and Wind Analysis Surface and buoy temperature observations
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Gulf Stream Location
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Results Day One Visible Satellite Image
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Day Two Visible Satellite Image
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Day Three Visible Satellite Image
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Omega Cross Sections Omega Cross Sections The time rate of change of pressure following an individual air parcel Since pressure decreases with height, negative omega indicates rising motion positive omega indicates sinking motion
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Day One Omega (Vertical Velocity) Pressure (mb) 3.5 km Location
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Day Two Omega (Vertical Velocity) Pressure (mb) 3.5 km Location
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Day Three Omega (Vertical Velocity) Pressure (mb) 3.5 km Location
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Why does it form? Convective Inhibition (J/kg) Time (UTC) May 25 May 26 May 27 09000-303-248 1500NA-606-179 2100NA-407-108 CINH - A measure of the amount of energy needed in order to initiate convection or how unlikely thunderstorm development may be The more negative the CINH in the sounding, the greater the atmospheric stability and lesser the chance of vigorous convection
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Synoptic Flow Day One: High pressure ridge to north, easterly flow Day Two: Ridge slides south, more westerly flow Day Three: Ridge to the south, westerly flow
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Why Does the Sea Breeze Cell Dominate Magnitude of temperature difference between the land and cold pool is much greater than the difference between the Gulf Stream and the cold pool Day one saw largest difference between Gulf Stream and cold pool, land and cold pool temperature difference remains fairly constant Peak on Day one
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Day One: Possible Scenario
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Summary Gulf Stream circulation cell was present on day one, but was not present on days two and three Easterly flow is helpful for Gulf Stream circulation cell formation Westerly winds cause the sea breeze cell to dominate over the smaller Gulf Stream cell Low and mid-level moisture and temperature profiles are important for cloud development
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Acknowledgements Professor Michael Splitt for all his knowledge and input Nicole Botto for the land – water temperature differences data Fellow MFP students for help with data collection
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Questions?
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