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Resolving the seasonal cycle of mixed layer physics and p Resolving the seasonal cycle of mixed layer physics and p

Resolving the seasonal cycle of mixed layer physics and p - PowerPoint Presentation

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Resolving the seasonal cycle of mixed layer physics and p - PPT Presentation

Seb Swart Sandy Thomalla amp Pedro Monteiro Chl a seasonal c ycle Thomalla et al 2011 Complex balance between light and nutrient limitation that drives higher production in SAZ ID: 286497

amp seasonal bloom mld seasonal amp mld bloom cycle saz summer wind scales fluor bvf light chl driven variability

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Slide1

Resolving the seasonal cycle of mixed layer physics and phytoplankton biomass in the SAZ using high-resolution glider data

Seb Swart, Sandy

Thomalla

& Pedro

MonteiroSlide2

Chl

-a seasonal

c

ycle

Thomalla

et al., 2011

Complex balance between light and nutrient limitation that drives higher production in SAZ

>> Sub-seasonal variability of MLD modulates this balance

Joubert

et al.,

submitted

Recent work highlights importance of seasonal to

sub-seasonal

forcing of ML on

PP

(Levy, Klein, 2009; Thomalla et al., 2011; Fauchereau et al., 2011)

The overall

Chl variance that is explained by the seasonal cycle (0-100%) was computed as the variance explained by the regression of Chl onto a repetition of the mean seasonal cycle.

SAZSlide3

High res

in situ MLD summer progression and variability

17 transects of

XBTs to derive MLD

Light - Fe threshold

(

Jourbert

et al., submitted)

SAZ

Underway

chl

-a south of AfricaSlide4

Well stratified

, punctuated by short winter mixSummer highly

reproducible but winter not

Dominated by heat fluxes.

STZ

APZ

MLDs are deep (±100m)

MLD is

seasonal = 57%

57%

17%

What do gridded datasets tell us?

Monthly EN3-derived Brunt-

Vaisala Frequency and MLD

14%Weak seasonal cycle = 14%Variable MLDs &

weak strat.Assoc with high wind var = 2.5 m.s-1SAZSlide5

HYPOTHESISHigh rates of PP in SAZ are a direct result of MLD variability at submeso-subseasonal scales

(around a threshold depth) that allows for alleviation of both light and Fe limitations at appropriate time scales for phytoplankton growth

Swart et al., 2012

…At

present we

cannot

do this without

continuously

sampling autonomous platforms!

Unless these time scales (sub-seasonal) are

correctly defined in terms physical – biogeochemical coupling, models will not accurately reproduce the seasonal cycle and hence predict future climate states Slide6

Gough Is.

STF

SAF

APF

Gough/Tristan Transect

GoodHope Line

Cape Town

Bathymetry (meters)

= Glider deployment & ship CTD station

= ship based underway measurements

±

2000 nm away…

So seasonal cycle experiment

September

2012 –

March

2013Slide7

SG573

SG574

SG543

SG575

SG542

Surface

– 1000m

1.4 km

horiz

res

2532 dives = 5064 profiles

537 days of sampling

+ ship process studySlide8

FLUORTEMP

SPRING

Bloom PRIMING PERIOD

SUMMER

Bloom Sustaining PERIODSlide9

FLUOR

BVF

T

fSlide10

Cyclone

Cyclone edge

Front edge

Intrusion

Submeso

filament -eddy

Strat

. (BVF)

0-100m & 100-300m

MLD

Fluor

Temp

Density

Poster by S. Nicholson et al:

PP sensitivities to

s

ubmeso dyn and subseas atm forcing Slide11

FLUOR

BVFSlide12

Wind

R

=0.52

Density

MLD

Fluor

Strat

. (BVF)Slide13

Spring – Summer MLD progression…a reminder of scales

5-hrly Glider

Monthly EN3

CFSR 7-daySlide14

Bloom initiations vary depending on the criteria used to define them. Different bloom initiations can be explained by different mechanisms (e.g. Sverdrup’s critical

depth, Taylor and Ferrari’s turbulent convection, Mahadevan’s eddy driven stratification)

>> The

response of the bloom onset to interannual and climatic

change will depend

strongly on which mechanism prevails,

eg. wind/features

2. In

S

pring, feature driven changes to the mixed drives early stratification and bloom initiations>> If climate models don’t include lateral processes they will overestimate

bloom initiation dates3. In Summer, wind driven adjustments to the mixed layer plays an important role in sustaining the summer phytoplankton

bloom by relieving Fe and light limitation at the appropriate time scales>> Highlight the importance of interplay between meso-submesoscale features

versus wind-buoyancy processes

in characterising the ML, productivity, timing

of the bloom and carbon exportConclusionsSlide15

Many thanks to the following people and collaborators!Geoff Shilling, Craig Lee &Eric D’Asaro at APL, UW

Derek &Andre at STS / SOERDCGrant Pitcher & Andre Du Randt, DAFF

Stewart Bernard,

Marjo Krug & Andy Rabagliati

, CSIRGavin

Tutt, DEA

IMT, SANAP, UCT, DEA & DAFF