lecture 8: coastal upwelling - department of mathematics, hkust

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Lecture 8: Coastal Upwelling The Physics of coastal upwelling Biological responses

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Page 1: Lecture 8: Coastal Upwelling - Department of Mathematics, HKUST

Lecture 8: Coastal Upwelling

• The Physics of coastal upwelling• Biological responses

Page 2: Lecture 8: Coastal Upwelling - Department of Mathematics, HKUST

Coastal UpwellingWind Stress

Coastal Upwelling Jet

Bottom Ekman Layer

Surface Ekman Layer

Page 3: Lecture 8: Coastal Upwelling - Department of Mathematics, HKUST

Processes in Coastal UpwellingWhen winds have a component blowing parallel to the coast, Ekman layer transport directed 90° to the right

Offshore surface transport lows sea level near the coastal, produces a pressure gradient which is directed normal to the shore and drives a geostrophic current along the coast

Flow field related to upwelling is directed at an angle away from the coast near the surface, parallel to the coast at mid-depth (below the Ekman layer but above the bottom boundary layer) and at an angle towards the coast in the frictional boundary layerat the bottom.

Page 4: Lecture 8: Coastal Upwelling - Department of Mathematics, HKUST

colder nutrient-rich waters from the deep ocean areuplifted onto the shelf and coastal upwelling jet is formed.

More than half of the world’s annual commercial fishing occur in the upwelling zone.

Page 5: Lecture 8: Coastal Upwelling - Department of Mathematics, HKUST

Five major coastal currents associate with upwelling area besides numerous coastal region, e. g. North South China Sea, coast off Vietnam

Page 6: Lecture 8: Coastal Upwelling - Department of Mathematics, HKUST
Page 7: Lecture 8: Coastal Upwelling - Department of Mathematics, HKUST

113 114 115 116 117 118 119

113 114 115 116 117 118 119

20

21

22

23

24

20

21

22

23

24

Temperature DIstribution on 10m layer in summer,2002

Horizontal distribution of water temperature at 10 m showing strong alongshore variability in upwelling on the shelf off NSCS (Guo, SOA)

wind

Page 8: Lecture 8: Coastal Upwelling - Department of Mathematics, HKUST

Relationships between the wind, Ekman drift and coast, as illustrated below, lead to the formation of Coastal Upwelling

Page 9: Lecture 8: Coastal Upwelling - Department of Mathematics, HKUST

Negative pressure gradient, dp/dx<0 (Pa>Pb), formed by the density contrast and sea level difference across the upwelling area, generates southward geostrophic current.

xy

Pa Pb

Page 10: Lecture 8: Coastal Upwelling - Department of Mathematics, HKUST

The width of coastal upwelling-the Rossby deformation scale

D: The distance of the upwelling front from shore, which moves offshore as upwelling progresses.

Ri (Rossby internal deformation scale): The width of the region where the interface rises to the sea surface.

Ri=(g’H)1/2/f

g’ is the reduced gravity, H is depth of the upper layer and f is Coriolis parameter.

ggρρρ 12' −

=

Page 11: Lecture 8: Coastal Upwelling - Department of Mathematics, HKUST

Variations in upwelling

• Time dependent• Space dependent

Page 12: Lecture 8: Coastal Upwelling - Department of Mathematics, HKUST

Spatial variability of upwelling:Ocean Surface Temperature on Sep. 5, 1994 as measured by satellite.

Page 13: Lecture 8: Coastal Upwelling - Department of Mathematics, HKUST

Sea Surface Temperature•By bottom topography:

Page 14: Lecture 8: Coastal Upwelling - Department of Mathematics, HKUST
Page 15: Lecture 8: Coastal Upwelling - Department of Mathematics, HKUST

Vectors of QuickScat wind stress (Pa) and MODIS SST (C) average over the cruise periods in 2000 and 2002

2000 2002

Page 16: Lecture 8: Coastal Upwelling - Department of Mathematics, HKUST

The topography (in meters)

in the northern South China Sea

Page 17: Lecture 8: Coastal Upwelling - Department of Mathematics, HKUST

zoomed area in the region

between Guangdong and Xiamen

305

338

372

The selected cross-shelf sections (dashedlines) are marked bytheir grid numbers.

The location where shelf isobaths protrudeshoreward is markedby SCI (shoreward convex isobaths).

Page 18: Lecture 8: Coastal Upwelling - Department of Mathematics, HKUST

(a) (b)

Daily mean (a) surface, (b) bottom velocity vectors (m s-1) ;

The 30 m and 50 m isobaths are shown as red and blue contour lines, respectively.

(c) (d)

(c) depth-integrated velocity magnitude (m s-1) and (d) surface elevation (m).

Page 19: Lecture 8: Coastal Upwelling - Department of Mathematics, HKUST

Day 10 Day 10

Day 30Day 30

Surface Bottom

Daily average surface (left column) and bottom (right column) σθ

(kg m-3) on days 10 and 30, showing the strong shoreward

advection near SCI and the subsequently eastward advection

of dense bottom waters between Shanwei and Shantou during upwelling.

Page 20: Lecture 8: Coastal Upwelling - Department of Mathematics, HKUST

u

v

ρ

0.4

0.3

0.1

0.2

0

-0.1

0.2

0.1

0

-0.1

-0.1

24.5

23.5

22.5

21.5

20.5

Across-shore sections of daily-averaged alongshore velocity, u (m s-1), cross-shore velocity v (m s-1) and density ρ (kg m-3) at lines 305 (Shanwei), 338 (Shantou) and

372 (Taiwan Shoals) on day 30

338

338

338

305

305

305

372

372

372

Page 21: Lecture 8: Coastal Upwelling - Department of Mathematics, HKUST
Page 22: Lecture 8: Coastal Upwelling - Department of Mathematics, HKUST

Alongshore velocity Water density

Page 23: Lecture 8: Coastal Upwelling - Department of Mathematics, HKUST
Page 24: Lecture 8: Coastal Upwelling - Department of Mathematics, HKUST

•By combined effects of time-dependent wind stress and coastline variation-------upwelling relaxation

Page 25: Lecture 8: Coastal Upwelling - Department of Mathematics, HKUST
Page 26: Lecture 8: Coastal Upwelling - Department of Mathematics, HKUST

Day 10 Day 13 Time

Wind Stress

1 Dyn.

Page 27: Lecture 8: Coastal Upwelling - Department of Mathematics, HKUST
Page 28: Lecture 8: Coastal Upwelling - Department of Mathematics, HKUST
Page 29: Lecture 8: Coastal Upwelling - Department of Mathematics, HKUST
Page 30: Lecture 8: Coastal Upwelling - Department of Mathematics, HKUST
Page 31: Lecture 8: Coastal Upwelling - Department of Mathematics, HKUST
Page 32: Lecture 8: Coastal Upwelling - Department of Mathematics, HKUST

Coastal trapped waves and other oscillations

• The local convergence or divergence along the coast increases or decrease local sea level, which leads to the formation of local pressure gradient

• The resulting currents from the local pressure gradient lead to the propagation of these local increased or decreased sea level (i.e. wave propagation)

Page 33: Lecture 8: Coastal Upwelling - Department of Mathematics, HKUST
Page 34: Lecture 8: Coastal Upwelling - Department of Mathematics, HKUST
Page 35: Lecture 8: Coastal Upwelling - Department of Mathematics, HKUST

Kelvin Wave

• largest amplitude at the coast, amplitude falls off exponentially towards the open ocean;

• Propagate in the direction with coastline on its right in the NH and on its left in the SH;

• Its existence requires coastline, but not shelf.

Page 36: Lecture 8: Coastal Upwelling - Department of Mathematics, HKUST

Coastal Trapped Waves

• Their existence requires region of shallow ocean between the coast and the deep ocean;

• Offshore and inshore movement of a water column during upwelling or downwelling on a sloping shelf below the Ekman layer is associated with a continuous change of potential vorticity due to the stretching and widening;

Page 37: Lecture 8: Coastal Upwelling - Department of Mathematics, HKUST
Page 38: Lecture 8: Coastal Upwelling - Department of Mathematics, HKUST
Page 39: Lecture 8: Coastal Upwelling - Department of Mathematics, HKUST

•Upwelling and primary production

Page 40: Lecture 8: Coastal Upwelling - Department of Mathematics, HKUST
Page 41: Lecture 8: Coastal Upwelling - Department of Mathematics, HKUST

Shantou

Page 42: Lecture 8: Coastal Upwelling - Department of Mathematics, HKUST

with river

Page 43: Lecture 8: Coastal Upwelling - Department of Mathematics, HKUST
Page 44: Lecture 8: Coastal Upwelling - Department of Mathematics, HKUST

without river

Page 45: Lecture 8: Coastal Upwelling - Department of Mathematics, HKUST

without river

Page 46: Lecture 8: Coastal Upwelling - Department of Mathematics, HKUST

Remarks about the upwelling-primary production

oThere is a time delay between the onset of the wind and the arrival of nutrient-rich water.

oThere has to be a quantity of nutrient-limited phytoplankton cells ready to respond the availability of nutrients

oThe high productivity results from the alternation of upwelling events. (upwelling brings nutrient, calm period, stratification develops, phytoplankton grows and multiplies)

Page 47: Lecture 8: Coastal Upwelling - Department of Mathematics, HKUST

•Upwelling and zooplankton

o Zooplankton organism, e.g. copepods, require longer time (weeks) to complete life cycle.

o Process is: adult copepods is upwelled to the surface from deep water during upwelling, their offspring thrive on the abundant phytoplankton and tend to be carried offshore. The peak value of zooplankton occurs when upwelling is weakened so that they can stay over the shelf.

Page 48: Lecture 8: Coastal Upwelling - Department of Mathematics, HKUST
Page 49: Lecture 8: Coastal Upwelling - Department of Mathematics, HKUST

Lower nitrate and chlorophyII-a, and higher zooplankton concentration are found during the periods after upwelling (or relaxation of upwelling and downwelling, e.g. June 22-30)

Page 50: Lecture 8: Coastal Upwelling - Department of Mathematics, HKUST

•Upwelling and fish

Upwelling favorable wind

Upwelling circulation

Upwelling nutrients

Bursts of Phytop.

Relaxing of upwelling winds

Build up of Zoo.

Landing of fish

Page 51: Lecture 8: Coastal Upwelling - Department of Mathematics, HKUST

Example of upwelling in California current

Page 52: Lecture 8: Coastal Upwelling - Department of Mathematics, HKUST

Bakun upwelling index:

fM

vC

E

da

τρτ

=

= 2

aρ is air density 0.00122 g cm-1, Cd is drag coefficient as 0.0026. The upwelling index is the simply the time average of Me for different part of coastal zone.

Page 53: Lecture 8: Coastal Upwelling - Department of Mathematics, HKUST
Page 54: Lecture 8: Coastal Upwelling - Department of Mathematics, HKUST
Page 55: Lecture 8: Coastal Upwelling - Department of Mathematics, HKUST

High surface Chl-a

Ekman Pumping and Primary Production in a Cyclone