Presentation is loading. Please wait.

Presentation is loading. Please wait.

Physical drivers of interannual variability in phytoplankton phenology

Similar presentations


Presentation on theme: "Physical drivers of interannual variability in phytoplankton phenology"— Presentation transcript:

1 Physical drivers of interannual variability in phytoplankton phenology
Harriet Cole1, Stephanie Henson2, Adrian Martin2, Andrew Yool2 1University of Southampton 2 National Oceanography Centre

2 Outline What is phenology and why is seasonality important?
Seasonality metric definition – bloom timing Basin-wide relationships between bloom timing and physical drivers Discussion – focus on subpolar North Atlantic and bloom initiation Future work 2

3 Phytoplankton bloom phenology
Date of annually occurring features Defined in bloom timing metrics Peak Point of slide: what is phenology, can sum up in metrics to measure objectively Initiation Termination

4 Why seasonality is important
Overlap with peak abundance in grazers Point of slide: important for food chain Match-mismatch hypothesis (Cushing, 1990) Time

5 Why seasonality is important
Overlap with peak abundance in grazers Carbon export – biological pump Seasonal variability linked to magnitude of flux and fraction that is labile/refractory Lutz et al. 2007 Point of slide: important for carbon export and climate

6 Key Questions Meteorological conditions modulate bloom magnitude
Subpolar North Atlantic - annual mean net heat flux, wind, TKE Spatially quite strong but not seen interannually (Follows and Dutkiewicz, 2002) Mean winter net heat flux and wind speed predictors for bloom initiation Irminger Basin (Henson et al. 2006) Does timing of change in physical environment influence bloom timing? – e.g. date the ML shoals/ML deepens Do physical processes drive all of bloom timing? Point of slide: bloom mag and weather mag, bloom timing and weather mag, bloom timing and weather timing 6

7 Critical depth vs. critical turbulence
Bloom starts when MLD becomes shallower than critical depth Critical turbulence Bloom starts when mixing rates become slower than phytoplankton growth and accumulation rates Net heat flux becomes positive (Taylor and Ferrari, 2011) Point of slide: examine two theories on bloom initiation, critical depth and critical turbulence Huismann et al. 1999

8 Bloom timing metrics GlobColour – satellite-derived chlorophyll
Merges SeaWiFS, MODIS and MERIS 1x1 degree resolution, 8 day composites, NASA Ocean Biogeochemical Model (NOBM) Assimilates SeaWiFS, 8 day composites, – Nerger & Gregg, 2008 High fidelity to seasonal characteristics – Cole et al. 2012 No gaps – error on bloom initiation (30 days), peak (15 days) from gaps in satellite data Initiation: rises 5% above annual median Peak: maximum chlorophyll value End: falls below 5% above annual median Siegel et al., 2002 Point of slide: how did I define bloom metrics +5% Annual median 8

9 Physical data sources MLD Net heat flux Irradiance
T and S profiles ( density change of 0.03 kg m-3 Net heat flux Satellite data + reanalysis products (NCEP/ECMWF) ( Irradiance PAR data from MODIS ( Average ML irradiance Point of slide: where did I get data

10 Average time series for North Atlantic
Point of slide: what does bloom initiation match with timing of changes

11 Physical timing metrics
Mixed layer depth Timing of MLD max, MLD shoaling PAR ML PAR starts to increase, fastest increase, MLD shallower than euphotic zone depth Net heat flux Timing that NHF turns positive – Taylor and Ferrari, 2011 Point of slide: what things am I correlating with bloom initiation and why am I doing that.

12 Results Bloom initiation more strongly correlated than peak and end with physical drivers Basin-wide response seen in subpolar N. Atlantic Patchy correlations in subpolar N. Pacific and S. Ocean Point of slide: broad results, how does BI and N.Atlantic fit in with broader context

13 North Atlantic latitudinal gradients
Bloom initiation r=0.76 r=0.69 Physical metric Point of slide: spatial gradients match well. Nhf the best compared to MLD r=0.58 r=0.86

14 North Atlantic interannual variability
6 30°x10° boxes in North Atlantic. Brackets indicate correlation coefficient is not statistically significant at the 95% confidence interval r=0.45 r=(0.36) Point of slide: Interannual variability correlations – NHF is the winner, PAR is not correlated (r=-0.12) (r=-0.013)

15 North Atlantic vs. North Pacific
Point of slide: correlations much stronger in N. Atlantic r=0.45 (r=-0.11)

16 Correlation map of bloom initiation and NHF turns positive
Point of slide: Broader spatial context. Basin wide response in North Atlantic, large patches of positive correlation in N.Pacific and S. Ocean Coherent patches

17 Discussion Bloom initiation – strongest relationship with changes in physical environment Suggests biological processes more important for peak and end timing Nutrient limitation, grazing, etc. NHF better than MLD for predicting start of bloom - critical turbulence vs. critical depth Basin-wide response seen in N. Atlantic both spatially and interannually Why different to N. Pacific and S. Ocean? Large scales – strong correlation, small scales - noisy Point of slide: what does this all mean. Peak and end are not driven by physics, NHF is better predictor, why is N Atl different

18 Next steps Impact of global warming on the seasonal cycle of phytoplankton Climate change-driven trends in bloom timing using biogeochemical models Final year – submitting in October Point of slide: thesis 18

19 Summary Seasonality metrics develop to estimate bloom timing
Correlated with timing of changes in physical environment – spatially and interannually Bloom initiation more strongly correlated than peak and end of bloom NHF better predictor than MLD for onset of bloom Basin-wide relationships weaker in N. Pacific and S. Ocean Point of slide: sum up results 19

20 Thank you for listening!
Acknowledgments GlobColour Project/ESA NOBM/Giovanni MODIS/NASA Coriolis Project WHOI OAflux Project Liége Colloquium – travel grant Thank you for listening! Questions? Point of slide

21 References Cole, H., S. Henson, A. Martin and A. Yool (2012), Mind the gap: The impact of missing data on the calculation of phytoplankton phenology metrics, J. Geophys. Res., 117(C8), C08030, doi: /2012jc Cushing, D. H. (1990), Plankton production and year-class strength in fish populations - an update of the match mismatch hypothesis, Adv. Mar. Biol., 26, Follows, M. and S. Dutkiewicz (2002), Meteorological modulation of the North Atlantic spring bloom, Deep-Sea Research Part Ii-Topical Studies in Oceanography, 49(1-3), Henson, S.A., I. Robinson, J.T. Allen and J.J. Waniek (2006), Effect of meteorological conditions on interannual variability in timing and magnitude of the spring bloom in the Irminger Basin, North Atlantic, Deep-Sea Research Part I-Oceanographic Research Papers, 53(10), , doi: /j.dsr Lutz, M.J., K. Caldeira, R.B. Dunbar and M.J. Behrenfeld (2007), Seasonal rhythms of net primary production and particulate organic carbon flux to depth describe the efficiency of biological pump in the global ocean, Journal of Geophysical Research-Oceans, 112(C10), C10011, doi: /2006JC Nerger, L. and W.W. Gregg (2008), Improving assimilation of SeaWiFS data by the application of bias correction with a local SEIK filter, Journal of Marine Systems, 73(1-2), , doi: /j.jmarsys Siegel, D.A., S.C. Doney and J.A. Yoder (2002), The North Atlantic spring phytoplankton bloom and Sverdrup's critical depth hypothesis, Science, 296(5568), , doi: /science Taylor, J.R. and R. Ferrari (2011), Shutdown of turbulent convection as a new criterion for the onset of spring phytoplankton blooms, Limnology and Oceanography, 56(6), , doi: /lo


Download ppt "Physical drivers of interannual variability in phytoplankton phenology"

Similar presentations


Ads by Google