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151 Cards in this Set
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- 3rd side (hint)
How does EUC drive production |
easterlies piling water in west causes slope of thermocline rising W to E; current follows bring deep nutrients up to east
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milankovitch cycles
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long period variations in orbit:
orbital vs elliptical path change in axial tilt spin axis tilt (move finger) |
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ENSO cause
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change in air pressure over tahiti/darwin australia, weaker trader winds
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oceanographic results of enso
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thermocline relaxes as less water piled up in west, less upwelling along coastal S. America
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atmospheric results of enso
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more warmer, spread out water, more sensible heat loss
wetter colder winters in SE US |
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estuarine requirements
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semi enclosed and coastal,
connected with sea saline |
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general estuarine flow
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salt gradient driven; fresh in at surface, deep saline outl
salt wedge strongest stratification, highest flow stronger at ebb tide |
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force balance for flow equation
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turn around
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barotropic PG
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higher sea surface where river input
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baroclinic PG
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increases with depth due to salinity
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estuarine/gravitational circulation
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balanced (subtitle) barotropic and baroclinic PG
drive circulation assumes no wind or bottom flow |
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wind and flow
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surface flow moves in direction of wind; deep flow moves opposite to maintain volume
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ETM
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convergence of river flux and landward circulation
accumulation of sediment and high turbidity @ limit of salt intrusion |
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balance between advection and turbulent mixing determines
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strength of vertical density gradient (board)
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length and stratification of estuary impacted by
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strength of river discharge;
stronger discharge, shorter estuary, greater stratification |
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coriolis causes
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outflow to deflect to right; can add or subtract from bay
Wind to N (CB) ekman transport out and high water at N end of bay |
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cold pool
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is there year round; isolated by summer stratification
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WBC
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advective dominance – high velocity, unstable, sheds eddies (warm core rings)
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warm core rings
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form (from instability) where GS separates from shelf (CH);
interact with shelf and help flush it |
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WBC w/out slope sea
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pump deep water onto shelf, colder in florida rules production
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warmer in AA, (CCDW) causes basal melt where polynyas form
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AACC against continent
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greatest basal melt
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EBC
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wind driving upwelling drives production at surface (WBC has production at bottom where water pumped over in absence of slope sea)
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THC Basics
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* heat lost from ocean at poles, cold water sinks and moves equatorward
* heat input at equator, cold water warms and moves poleward |
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THC Basic Pathway
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* upwells and returns in indian
* upwells and returns in mid lat pacific across northern Australia (return stream joins indian ocean stream) |
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Cross Section of Atlantic, top to bottom
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* NACW, AAIW, NADW, MIW NABW East, AADW AABW west
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dense water forms by
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* removal of heat
* ice formation * evaporation |
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* Source/Formation Region:
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* area of ocean where water mass acquires its characteristic properties
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* Conservation property
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* (apply only below ocean surface mixed layer ~1000m)
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* Water type:
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* body of water with a common formation history, having its origin in a particular region, occupy finite volume (point in TS space) may not exist (big average)
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* Source water type
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* water type that corresponds closely to parties of water mass in source region.
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* Water mass:
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* body of water with common formation history, origin in particular region
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convection
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* deep and bottom waters
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subduction
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* mode and intermediate waters
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subsurface mixing
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* circumpolar deep water
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ocean ventilation
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* where deep water acquire’s characteristics
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consolidation
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* mixing within mater mass; reduces standard deviation without changing mass (reduces TS variability)
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mixing
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* between water masses; new combinations; identify contribute water masses and determine relative scale (happens through double diffusion, molecular level)
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absorption
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* ater mass disasters by mixing with another; Med into NADW
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transformation
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* change to another water mass by subsurface mixing CDW
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NADW formed
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* in Labrador (little), Greenland, Norwegian Sea
* 2–4ºC; 34.9 – 35 psu |
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no bottom water formation in pacific?
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not salty enough
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* trong MOC mixes with relatively fresh Arctic,
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* keeping salinity relatively high; allows for formation of NADW
* freshening of arctic will weaken MOC |
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* Climate feedback MOC
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* without redistribution of heat by slower circulation, polar water colder, ice grows and becomes saltier
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AABW more dense than NADW because
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* more dense because ‘less entrainment' with surface
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polynya defn and formation
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* latent heat formation: ice formed and wind blows away repeatedly
* sensible heat formation: ice melts from below (Antarctic water) upwelling |
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* Polynyas form and freeze
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forming AABW
* this collections on antarctic shelf and eventually spills into deep water * this foredeepend shelf is closer to land because ice sitting on it * .4–1ºC; 34.6 – 34.9 psu |
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MIW
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* Mediterranean net evaporation, tongue flows over Gibraltar strait
* 5–10ºC; 35.5–35.9 psu * return path of THC; important source of salinity for NADW formation * |
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theory for deep circulation principles
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1. Supply of cold dense waters by itself doesn’t drive deep circulation; need sinking near poles to be balanced by rising water
2. Permanent thermocline depth ~ constant. Net input of heat at equator, so thermocline can only remain constant if there is a source of cold water from below (entrainment and mixing). 3. Turbulent mixing and not density differences drives the deep circulation. This requires overturning (mixing) hence MOC |
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theory for deep circulation details
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* stratification up (input heat and freshwater), speed down
* NH moving toward equator increases positive vorticity * So friction can only balance planetary vorticity of an equatorward flow along WBC * |
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MOC moves heat received across equator so
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* ~ flux of 20 Sv
* 35% of insolation received at 40ºN is put into North Atlantic through conversation from warm surface to cold NADW * so 5º colder in NA if no MOC; slowing of ^ could cause ice to reform in Norway * |
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Water mass general characteristics
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* NA: open to north, limited seasonal sea ice, freshwater sources (rivers)
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* NADW, GSW, LSW (Labrador Sea Water), MSW STO
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* high salinity, low temp, high O2
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* AAIW SI
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* low salinity, high oxygen
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* AABW STO
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* high salinity, low temperature, average O2
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* Subtropical underwater:
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* low oxygen; consumed though respiration, less mixing
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* AABW blocked
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* on eastern side blocked by Walvis Ridge
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* Catabatic winds
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* in AA drives off ice and forms polynyas
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* TS Distribution for world oceans; most is 34.6 ppt and ~ 1.5ºC (potential)
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* Atlantic, saltiest and mid temp
* Indian, less salty and cooler * Pacific, fresh and warmer |
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AACC
* formed of |
* 40/55 cm/s; 40–45 Km wide; locations?
* transport through drakes passage ~ 120 Sv * boundary between mid/high latitude waters? |
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* AABW moves
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* clockwise around S pole between 70 N and 70 S
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intermediate/node waters
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* subducted @ polar front
* Winds W to E; ekman transport north |
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shelfs and AABW
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* High Salinity Shelf Water precursor of AABW
* Ice Shelf Water formed under ice shelf (high pressure allows it to be water below it’s freezing point) * Circumpolar Deep Water cools and freshens all oceans as they enter |
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pacific basin
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* composed of many little basins made of pacific common water; mix of everything
* south west pacific about as from from source waters as you can get; oldest and O2 depleted * |
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Internal Osciallation formula
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combined coriolis parameters
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internal oscillation
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ocean impulsively started (cold fronts)
no slope/pressure motion in circle |
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geostrophic flow
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flow is balance between coriolis and pressure
pressure directs flow along pressure gradient from high to low; coriolis acts opposite pulls flow R of Low pressure ALONG CONSTANT PRESSURE/SSH |
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density decreases west to east NH
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dividing by smaller, speed increases north as move up water column
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pressure increases west to east NH
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flow north; greater increase greater speed
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necessary condition for observed gulf stream and implications
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it must be a meter higher over 50 km; if it slows slope will change and it will flood here
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potential density
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density of water moved adiabatically to ocean surf; so effects of compressibility removed
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specific volume
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1/density
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specific volume anomoly
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difference in specific volume of sample and open ocean (no need for potential density)
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dynamic height
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measure of potential energy change between two pressure levels
measuring the energy (divide by gravity for height) required to maintain the pressure between two surfaces based on density fluctuations. More dense, less height/energy |
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dynamic height anamoly
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change in dynamic heights between two stations at same pressure is proportional to horizontal pressure change.
subtract standard ocean (1/density at S 35, T 0, P same) |
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hydrostatic and rearrangment formula
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dP/dz = –grho
alpha (1/rho) dP = –gdz –gdz = D ynamic height (integrate to solve) |
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horizontal and vertical force balance in ocean
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horizontal geostrophic: pressure vs coriolis
vertical hydrostatic: gravity * desnity (weight) down by vertical pressure gradient up |
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quasi geostrophic
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allowing small changes in pressure and flow
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turbulent friction
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10 – 100 meters ekman force matters
mixed layer wind blowing over surface exterts tangential force (surface stress, wind acts parallel to ocean surface) |
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wind causes water to move
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at linearly decreasing speed with depth
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wind forcing with coriolis
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surface current 45degrees to right of wind in NH
ekman spiral; Newton's third law (equal and opposite force) moving down water column, speed slows a deflects a little more to right |
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2 forces acting on vertically integrated column
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wind and coriolis; net transport in friction layer 90 degrees to right of wind; just like 90 degrees right of pressure gradient
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winds blow
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along coast, upwelling because water transport is offshore
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upwelling with two density layers
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north wind, transport offshore
establishes a pressure gradient (higher where more water offshore) net flow now north, same as wind (because of geostrophic) more dense water fills in where water lost at coast. slowly reverses pressure gradient and thus transport. |
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bottom friction
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pressure constant but water slows. thus coriolis must be weakening. so transport shifts to the direction of the pressure gradient (low to west, flow to west)
transport is thus left of water above it. |
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ekman pumping
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wind is blowing on one spot; because of coriolis in N there will be more transport to the right of this spot and downwelling; less to left and upwelling.
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equator out wind direction
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east between 30 and 0: trades
west between 60 and 30: westerlies east between 90 and 60: polar easterlies |
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wind cells
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NH
Hadley 0/30 counterclockwise Ferrel 30/60 clockwise Polar 60/90 counterclockwise |
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circulation caused by wind pattern
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trades and westerlies; ekman push water into center gyrating fashion. sea level rises in center, thermocline/pycnocline descends (density decreases, faster)
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vorticity
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instrinsic spin of fluid
zeta = chaning N/S velocity as EW direction – chging speed in EW as changing NS direction |
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planetary vorticity
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f = 2 thingy sin (lat)
coriolis |
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potential vorticity
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total spin of fluid column divided by height
conserved following flow if no friction or forcing (so if f changes with latitude zeta or H must) |
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wind adds ______ vorticity because
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negative, clockwise ekman (WE (+) direction, flow NS (–) +*– = –); – (NS direction, Flow E to W so –– +)
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eastern boundary vorticity dynamics
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north; negative vorticity balanced as you decrease latitude and decrease f
south; negative vorticity balanced by continent friction |
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western boundary vorticity dynamics
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south; negative vorticity balanced decrease in latitude
north; negative vorticity increases as you increase latitude; unbalanced |
result because gyre doesn't move: negative vorticity expressed as increase in speed along boundary (western intensification) that results in enough friction to balance vorticity
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conservation of PV
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conserved following flow if no friction or forcing (because it's energy)
we assume isobaric (no depth change) when working with it so change in latitude must correspond to change in relative vorticity |
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hydrostatic pressure
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vertical force opposing gravity
pressure force change in w/ depth balances weight of fluid (P = rho*g*depth) |
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horizontal pressure gradient
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change in accel = –gS(difference in height)/L (distance separating)
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horizontal density gradient
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accel = –g (rho 2 – rho 1) *h/rhoL
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coriolis vs centrifugal
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while in motion earth moves you right in coriolis
spinning earth throws anything away from axis |
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coriolis force =
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f*u
f = 2 rate of spin *sin (latitude) about 10^–4 at midlatitudes |
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friction
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Fx = –K (deriv A/deriv X)
Ficks law; diffusive flux in x direction = diffusivity (constant) *change in concentration in changing x direction |
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if diffusivity flux varies in space
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take derivative of diffusive flux (a/t)
= K (second derivative of A/second derivative of x) factor out deriv/derivX for molecular diffusivity |
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turbulent vertical velocity
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change in correlation of speed fluctuations
average compass direction speeds correlated with vertical movement higher wind speed more vertical mixing vertical change of vertical correlation |
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reynolds averaging
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to separate mean velocity (u bar) from turbulence (u prime)
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to make average flux equation
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average of each term and add 0 acceleration (boussinesq)
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reynolds number
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compares inertial forces (advective) forces to viscous (Friction) forces
Re = UL/v when large, molecular viscosity doesn't matter |
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rossby number
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compares inertial forces to coriolis
U^2/L : fU Ro = U/Lf small rossby means coriolis important (is in ocean) |
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ekman number
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Coriolis to vertical turbulent viscosity
fU=Kh (U/H^2) Kh/H^2f kh = .01; matters at surface, not at depth |
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geostrophic balance
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pressure gradient must balance coriolis force
it does ~ 1 m rise in sea surface over 100 km balances fV = gS/L solve for S using v = 1m/s and L = 100 Km (gulf) |
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kinematics vs dynamics
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analysis of motion withou forces vs with forces
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newton's 1st law
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inertia; remains in motion stays in motion
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newton's 2nd law
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f = ma
in ocean, acceleration is produced by net forces |
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newton's 3rd law
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if one object exerts a force on a second object, then second exerts and equal and opposite force
in ocean think about pressure gradient up and down and |
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unsteady vs steady motion
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unsteady time dependent, changes with time; non zero acceleration
steady is independent of time; forces balanced; no acceleration |
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4 forces interior to ocean
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gravity
pressure gradients coriolis friction |
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brownian motion
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thermal agitation of fluid molecules
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fick's law def
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mixing proportional to spatial gradient of the property
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if _____ is being diffused the constant is called the _________
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momentum, viscosity
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Incoming heat vs outgoing heat
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all outgoing in top millimiter
incoming begins 10^–6 m more until 1 then back down |
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Wien's Law
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wavelength of maximum transmission is inversely proportional to the absolute temperature
lambda max = b/k b=cw=constant=2.9*10^6 nm * K |
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Stefan Boltzmann Law
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all bodies radiate energy at a rate proportional to 4th power of absolute temp:
Qb = CsK^4 Cs = 5.6*10^–8 W/m^2 K^4 |
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relation between wien and stefan boltzmann
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type of wavelength emitted vs amount of energy radiated
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solar constant
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flat plate receives 1368 watts/m^2
earth receives 342 watts/m^2 |
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wavelengths emitted by sun
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50% visible; 10% UV remainder 40%
Max red because 5500K is sun |
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less irradiance reaches surface of earth because
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absoption by atmosphere particles
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average planetary albedo
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30%
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Ice albedo feedback:
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More ice formation, greater albedo, less absorbed radiation, more cool oceans, MORE ice formation (positive feedback)
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ocean radiates vs absorbs where difference?
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400 w/m^2 emitted; half of 342 absorbed; rest is effective back radiation
effective back radiation: atmosphere traps longer wave infrared (lets through short from sun) about 50 –75 w/M^2 |
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OLR
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outgoing long wave radiation decreases from equator poleward
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latent heat loss
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energy to break hydrogen bonds and evaporate; about 100W/M^2 greatest at equator and in gyres
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conservative materials have no
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sources or sinks
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absorption by gas
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UV = o3
Short infrared 02, medium infrared water, long infrared CO2 |
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factors affecting Qs
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height of sun
length of day albedo attenuation: clouds, path through atmosphere (height of sun dependent) gas molecules, aerosols, dust |
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net infrared flux depends on
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cloud thickness (thicker less heat to escape)
cloud height (clouds radiate heat towards earth as black body, high colder than low) |
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relative atmospheric warming
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44 from earth 20 from sun
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molecular vs turbulent diffusion coefficeint
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1.5x10^–9 m^2/s
1x10^–2 |
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Reynolds number
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inertial to viscous, velocity scale x length scle / viscosity of substance
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salt equation for turbulent flow
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flow out equals in speed of flow in all directions + vertical turbulent flux change in depth * Az *change in salinity with depth (gradient
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Box Model Knudsen's RElationship
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Vi+R+P=E+Vo
R+P–E = x Vo–Vi = X with conservation of salt ViSiPi = VoSoPo Vi=X(So/Si–So) Vo=X(Si/Si–So) |
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Residence Time
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Tres=Vol/Flux In
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SST Up
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Qb down; Qe down; Qh up
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decreased relative humidity
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Qe up; Qb up
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increased wind speed
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Qe up; Qh up
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decreased air temperature
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Qh up; Qb up
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effective back radiation is difference between
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long way energy emitted from sea surface minus long wave energy received from atmosphere
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night/day b radiation
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cloud cover at night, frost results from radiative cooling whereas on clear nights it does not
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Qb
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net rate of heat loss by sea as long wave radiation to the atmosphere and space
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decreased air/water temp difference
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Qh down Qb down (less humidity)
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thermal vs salinity diffusivity
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thermal faster 1.5x10^–7
salinity 1.5 *10^–9 |
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increase/decrease in SST
increase/decrease AirT |
increase/decrease in rel humidity
decrease/increase in " |
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avg langley/day over course of year
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350 |
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