SLIDE 1 Trevor J McDougall
Royal Society of Tasmania, 4th November 2014
What has the Ocean got to do with Climate?
Ocean Physics, School of Mathematics and Statistics
SLIDE 2
Acknowledgements
Gary Brown (Uni Adelaide, Princeton) Stewart Turner (Uni Cambridge, ANU) Paul Linden (Uni Cambridge) Peter McIntosh (CSIRO, Hobart) Steve Griffies (NOAA GFDL, Princeton) Nathan Bindoff (Uni Tasmania, Hobart) Bill Dewar (Florida State Uni) Chris Garrett (Uni Victoria, Canada) Juergen Willebrand (GEOMAR, Kiel) Peter Gent (NCAR, Boulder) Rainer Feistel (IOW, Warnemunde) Rich Pawlowicz (UBC, Vancouver) Dan Wright+ (BIO, Canada) Richard Greatbatch (GEOMAR, Kiel) John Church (CSIRO, Hobart) Bernadette Sloyan (CSIRO, Hobart) Paul Barker (UNSW Sydney) David Jackett+ (CSIRO, Hobart) Yuzhu You (Uni Sydney) Andreas Klocker (Uni Tasmania) Jan Zika (NOC, Southampton) Felicity Graham (Uni Tasmania) Sjoerd Groeskamp (Uni Tasmania) Stefan Riha (UNSW Sydney) Yuehua Li (UNSW Sydney) David Woolsey (UNSW Sydney)
SLIDE 3
The ocean’s role in climate
SLIDE 4
The northward flux of heat
SLIDE 5
The horizontal ocean circulation
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The vertical ocean circulation
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The vertical ocean circulation
SLIDE 10
The layered nature of the ocean
SLIDE 11
Vertical mixing by internal wave breaking
(the Standard Model)
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The ocean’s role in climate
Diapycnal spread of a tracer at 300m Kv=0.17 x 10-4 m2s-1 Ledwell et al. 1998
SLIDE 13
Climate Change
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The ocean’s role in climate
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The ocean’s role in climate
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Emissions versus concentrations
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The ocean’s role in climate
SLIDE 18
Global emissions pathways to give us a 67% chance of not exceeding 2oC warming
SLIDE 19
Historical versus present carbon emissions
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The ocean’s role in climate
SLIDE 22
Our future climate is up to us:- will we be rational or stupid?
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The ocean’s role in climate
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The ocean’s role in climate
SLIDE 25
In October 2014 the European Union agreed to cuts its greenhouse gas emission by 40% by 2030 (compared to the emissions of 1990).
Share of energy from renewable sources in 2012 (%)
SLIDE 26
Back to the Ocean
SLIDE 27
Energy content changes in different components of the Earth system for two periods (1961–2003 and 1993–2003).
SLIDE 28
The ocean’s role in climate
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SLIDE 30 Ocean Heat Content, integrated from the surface 2000 metres depth in the global ocean.
X Chen, and K Tung Science 2014;345:897-903
SLIDE 31
Argo
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The ocean’s role in climate
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The ocean’s role in climate
SLIDE 35
The ocean’s role in climate: some of my research
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The ocean’s role in climate: some of my research
SLIDE 37
My first publication; a photograph of nothing.
SLIDE 38
When an under-sea oil well “blows out”
SLIDE 39
When mixing causes un-mixing
SLIDE 40
What is an appropriate average velocity?
McDougall and McIntosh (1996, 2001)
SLIDE 41
What is an appropriate average velocity:- Transport of water of given density classes
McDougall and McIntosh (1996, 2001)
SLIDE 42
The vertical ocean circulation
SLIDE 43
Vertical mixing by internal wave breaking
(the Standard Model)
SLIDE 44
Cabbeling and Thermobaricity
This is a “parcel view” of lateral thermobaricity and cabbeling Cabbeling occurs when the water parcels intimately mix at the molecular level. The diapycnal thermobaric advection occurs as the parcels move together, before mixing. This advection is made irreversible by the molecular mixing.
SLIDE 45 Cabbeling and Thermobaricity
SLIDE 46
Thermobaricity
Thermobaric vertical advection through an surface
(with average pressure of 1400 dbar)
SLIDE 47
The local direction of neutral mixing is the plane that is normal to
The ill-defined nature of “neutral surfaces”
SLIDE 48
The helical nature of neutral trajectories
For a neutral surface to be well-defined, Neutral Helicity, must be zero everywhere on the surface.
SLIDE 49
The ill-defined nature of “neutral surfaces”
Neutral helicity can be written as
where the thermobaric coefficient is
H being zero implies
(a) that the line lies in an isobaric surface, and (b) that contours of p and in a neutral tangent plane are parallel, and (c) that and data in an isobaric surface describe a line (rather than an area) on the diagram.
SLIDE 50
(a) Zero helicity requires that lie in the p surface since has to be zero.
Scanned map of p and theta on an approximately neutral surface.
The ill-defined nature of “neutral surfaces”
SLIDE 51
The diagram for the Atlantic, 250 dbar to the bottom
Colour is latitude; blue in the south, green at the equator, red in the north.
While this plot of all the data from both the North & South Atlantic looks “solid” or “full” on the diagram, …
SLIDE 52
Atlantic Ocean, 500dbar to 3300dbar
The global ocean is quite “thin” in space.
SLIDE 53
another view of the Atlantic
Atlantic Ocean, 500dbar to 3300dbar
SLIDE 54
Figure from David
(c) Zero helicity requires that the contours of constant and be parallel in an isobaric surface, that is,
The ill-defined nature of “neutral surfaces”
SLIDE 55
Vertical motion due to the ocean not being 100% “skinny”
Because the ocean is not totally “empty” in space, fluid can migrate vertically through any “density” surface simply by cork- screwing its way along helical neutral trajectories without the need for any dissipation of mechanical energy. If the global ocean volume in space were not so tiny, it would make no sense to study diapycnal mixing, tidal mixing, and diapycnal tracer diffusion.
SLIDE 56
Diapycnal flow caused by Neutral Helicity
SLIDE 57 The spatial variation of the vertical motion caused by four strange mixing processes
Sum of vertical transports caused by the nonlinear equation
- f state on an surface (average pressure = 1400 dbar)
SLIDE 58 The zonally-averaged dianeutral velocity
Zonal mean of the sum of four different vertical transports, each caused by the nonlinear nature of the equation of state . => These nonlinear processes are larger than the “standard model”
- f breaking internal waves in the Southern Ocean.
SLIDE 59
The globally-integrated dianeutral transports
Vertical profile of globally integrated transports caused by neutral helicity (its spatial form, green), cabbeling (blue), thermobaricity (red), and their sum (black). => The nonlinear equation of state causes downwelling of about 6 Sv, mostly in the Southern Ocean.
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What are these “density” surfaces?
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An Atlantic cross-section showing various types of density surface
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Improvements in the fictitious diapycnal diffusion of density (Veronis error)
SLIDE 63
Specific heat capacity at constant pressure, cp (J kg-1 K-1) at p = 0 dbar
What is “heat” in the ocean?
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What is “heat” in the ocean?
SLIDE 65 A new internationally adopted definition of seawater in terms
Conservative Temperature, TEOS-10
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The ocean’s role in climate
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Inverse model estimates of ocean mixing and circulation
SLIDE 69
Revision: the key messages of this talk
SLIDE 70
Energy content changes in different components of the Earth system for two periods (1961–2003 and 1993–2003).
SLIDE 71 Ocean Heat Content, integrated from the surface 2000 metres depth in the global ocean.
X Chen, and K Tung Science 2014;345:897-903
SLIDE 72
The ocean’s role in climate
SLIDE 73
The ocean’s role in climate
SLIDE 74
Global emissions pathways to give us a 67% chance of not exceeding 2oC warming
SLIDE 75
The layered nature of the ocean
SLIDE 76
Vertical motion due to the ocean not being 100% “skinny”
Because the ocean is not totally “empty” in space, fluid can migrate vertically through any “density” surface simply by cork- screwing its way along helical neutral trajectories without the need for any dissipation of mechanical energy. If the global ocean volume in space were not so tiny, it would make no sense to study diapycnal mixing, tidal mixing, and diapycnal tracer diffusion.
SLIDE 77