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Past and Future Climate Simulation Lecture 3 – GCMs: parameterisations (1) From last time – discretising the advection equation (2) Parameterisations: clouds/precip, land surface, dust, the oceans. (3) Implementation: boundary conditions, initial conditions. (4) Model output and model-data comparison (5) Experimental Design (6) Model tuning
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Past and Future Climate Simulation Lecture 3 – GCMs: parameterisations (1) From last time – discretising the advection equation (2) Parameterisations:

Mar 28, 2015

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Page 1: Past and Future Climate Simulation Lecture 3 – GCMs: parameterisations (1) From last time – discretising the advection equation (2) Parameterisations:

Past and Future Climate Simulation

Lecture 3 – GCMs: parameterisations

(1) From last time – discretising the advection equation

(2) Parameterisations: clouds/precip, land surface, dust, the oceans.

(3) Implementation: boundary conditions, initial conditions.

(4) Model output and model-data comparison

(5) Experimental Design

(6) Model tuning

Page 2: Past and Future Climate Simulation Lecture 3 – GCMs: parameterisations (1) From last time – discretising the advection equation (2) Parameterisations:

2 main parts to atmospheric GCM:

1) Adiabatic (no heat exchanged) – e.g. advection, surface friction.

2) Diabatic (heat exchanged) – e.g. radiation, boundary layer, clouds

Adiabatic advection of a tracer. E.g. a volcanic ash cloud moving around the equator, in a wind of constant speed, u:

180E 180E 180E180W 180W 180W

u

Example of numerics – atmospheric tracer

Page 3: Past and Future Climate Simulation Lecture 3 – GCMs: parameterisations (1) From last time – discretising the advection equation (2) Parameterisations:

name A B C D E F G H I J

longitude 0 36E 72E 108E 144E 180E 216E 252E 288E 324E

Initial Concentration

0 1 0 0 0 0 0 0 0 0

U=0.1A0=0, B0=1, C0=0,……

A1=0, B1=B0-0.1, C1=C0+0.1,D1=0,……name A B C D E F G H I J

longitude 0 36E 72E 108E

144E 180E 216E 252E 288E 324E

Initial Concentration 0 1 0 0 0 0 0 0 0 0

Concentration after 1 timestep

0 0.9 0.1 0 0 0 0 0 0 0

Concentration after 2 timesteps

0 0.81 0.18 0.01 0 0 0 0 0 0

Excel demonstration

Page 4: Past and Future Climate Simulation Lecture 3 – GCMs: parameterisations (1) From last time – discretising the advection equation (2) Parameterisations:

2 main parts to atmospheric GCM:

1) Adiabatic (momentum equation, last lecture)

2) Diabatic (heat exchanged) – e.g. convection, radiation (including clouds, greenhouse gases, aerosols), precipitation, surface energy balance. All parameterisations.

e.g. precipitation:

If (relative humidity > 85%) then

precipitation = (relative humidity - 85%)*constant

relative humidity = 85%

e.g. convection:

If (temperature gradient > 10oC/km) then

clouds = 1

temperature gradient = 10oC/km

precipitation

(2) Parameterisations

Page 5: Past and Future Climate Simulation Lecture 3 – GCMs: parameterisations (1) From last time – discretising the advection equation (2) Parameterisations:

e.g. land surface and turbulence:

Page 6: Past and Future Climate Simulation Lecture 3 – GCMs: parameterisations (1) From last time – discretising the advection equation (2) Parameterisations:
Page 7: Past and Future Climate Simulation Lecture 3 – GCMs: parameterisations (1) From last time – discretising the advection equation (2) Parameterisations:

(1) Potential dust source regions

e.g. aerosols (here, dust):

Page 8: Past and Future Climate Simulation Lecture 3 – GCMs: parameterisations (1) From last time – discretising the advection equation (2) Parameterisations:

(2) Wind speed….

~ u3 with a threshold….

Page 9: Past and Future Climate Simulation Lecture 3 – GCMs: parameterisations (1) From last time – discretising the advection equation (2) Parameterisations:

(3) Gusts….

convection

(4) Soil moisture….

(5) Wet deposition…

Page 10: Past and Future Climate Simulation Lecture 3 – GCMs: parameterisations (1) From last time – discretising the advection equation (2) Parameterisations:

(6) Dry deposition…(7) Evaluation

Page 11: Past and Future Climate Simulation Lecture 3 – GCMs: parameterisations (1) From last time – discretising the advection equation (2) Parameterisations:

Simulate just the uppermost approx 50m of the ocean (homogeneous slab of water).

Typically, atmosphere calculates the surface energy fluxes for each gridbox (net-solar, net-infrared, sensible, latent heats). The sum will not be zero; this is the net energy flux at the surface. If it is positive, the ocean absorbs this and warms up appropriately. If it is negative the ocean will cool down.

Need to parameterise ocean heat transport! Therefore no good for time periods/climates very different from modern.

1) 2)

e.g. oceans:

Page 12: Past and Future Climate Simulation Lecture 3 – GCMs: parameterisations (1) From last time – discretising the advection equation (2) Parameterisations:

(3) Configuring Models – boundary conditions/initial conditions

Boundary Conditions: Prescribed (by the user) fields. e.g. land- sea mask.

The model can not change these.

May be time-varying (e.g.SST).

Initial Conditions: Fields used for initialising the model.

After first timestep, model calculates. e.g. surface temperature

Page 13: Past and Future Climate Simulation Lecture 3 – GCMs: parameterisations (1) From last time – discretising the advection equation (2) Parameterisations:

Land-sea mask

Boundary conditions

Page 14: Past and Future Climate Simulation Lecture 3 – GCMs: parameterisations (1) From last time – discretising the advection equation (2) Parameterisations:

Orography

Page 15: Past and Future Climate Simulation Lecture 3 – GCMs: parameterisations (1) From last time – discretising the advection equation (2) Parameterisations:

Sub-gridscale orography

Page 16: Past and Future Climate Simulation Lecture 3 – GCMs: parameterisations (1) From last time – discretising the advection equation (2) Parameterisations:

Bathymetry

Page 17: Past and Future Climate Simulation Lecture 3 – GCMs: parameterisations (1) From last time – discretising the advection equation (2) Parameterisations:

Surface albedo (for models not predicting vegetation)

Page 18: Past and Future Climate Simulation Lecture 3 – GCMs: parameterisations (1) From last time – discretising the advection equation (2) Parameterisations:

Sea surface temperatures (for models without an ocean)

Page 19: Past and Future Climate Simulation Lecture 3 – GCMs: parameterisations (1) From last time – discretising the advection equation (2) Parameterisations:

Incoming solar radiation

Page 20: Past and Future Climate Simulation Lecture 3 – GCMs: parameterisations (1) From last time – discretising the advection equation (2) Parameterisations:

Greenhouse gases, aerosols

Page 21: Past and Future Climate Simulation Lecture 3 – GCMs: parameterisations (1) From last time – discretising the advection equation (2) Parameterisations:

Initial conditions

Surface Temperature Pressure in mid-atmosphere

Cloud cover Soil moisture

+ for ocean: temp,salinity,u,v,seaice

Page 22: Past and Future Climate Simulation Lecture 3 – GCMs: parameterisations (1) From last time – discretising the advection equation (2) Parameterisations:

(4) Model output and model-data comparison

Page 23: Past and Future Climate Simulation Lecture 3 – GCMs: parameterisations (1) From last time – discretising the advection equation (2) Parameterisations:

Produce a ‘climatology’

Page 24: Past and Future Climate Simulation Lecture 3 – GCMs: parameterisations (1) From last time – discretising the advection equation (2) Parameterisations:

Model-data comparison…

Page 25: Past and Future Climate Simulation Lecture 3 – GCMs: parameterisations (1) From last time – discretising the advection equation (2) Parameterisations:

Surface Temperature: observations

Surface Temperature: HadCM3

How good are GCMs?(1) temperature

Page 26: Past and Future Climate Simulation Lecture 3 – GCMs: parameterisations (1) From last time – discretising the advection equation (2) Parameterisations:

Precipitation: observations

Precipitation: HadCM3

Seaice: observations vs models

How good are GCMs?(2) Precip and seaice

Page 27: Past and Future Climate Simulation Lecture 3 – GCMs: parameterisations (1) From last time – discretising the advection equation (2) Parameterisations:

How good are GCMs?(3) El Nino

Page 28: Past and Future Climate Simulation Lecture 3 – GCMs: parameterisations (1) From last time – discretising the advection equation (2) Parameterisations:

(5) Experimental Design

Key concept: Testing hypotheses.

Typically, a ‘control’ + a number of ‘sensitivity studies’

• Modify a boundary condition…

“If everyone painted their roofs white, could this mitigate against global warming?”

• Modify an internal parameter…

“Can the fact that all models predict too-cold poles in deep-time palaeoclimates be due to the lack of anthropogenic aerosols?”

• Modify an initial condition…

“Was the Sahara bistable in the mid-Holcoene, 6,000 years ago?”

• Change a parameterisation…

“Does poor representation of clouds in models result in poor ENSO simulation?”

• Change the whole model…

“Which is the best model to use for future climate prediction?”

Page 29: Past and Future Climate Simulation Lecture 3 – GCMs: parameterisations (1) From last time – discretising the advection equation (2) Parameterisations:

(6) Model Tuning

We know that internal model parameters affect the control climate produced by a model…often these are not well constrained by data.

Therefore we can legitimately ‘tune’ the model towards observations of modern climate by ‘tweaking’ these parameters…

For a small number of parameters, we can cover ‘parameter space’ well…but….N=Ax , where N is number of simulations, A is how well we sample the parameter space, and x is the number of parameters….soon become unmanageable.

So, various approaches, including random sampling…..

Page 30: Past and Future Climate Simulation Lecture 3 – GCMs: parameterisations (1) From last time – discretising the advection equation (2) Parameterisations:

And ‘latin hypercube’ sampling…..

Skill score generated, and then experiments ranked...

Page 31: Past and Future Climate Simulation Lecture 3 – GCMs: parameterisations (1) From last time – discretising the advection equation (2) Parameterisations:

Tuned model outperforms original model…..

observations tuned model original model