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A revision of the Earth’s energy balance framework A. E. Dessler Dept. of Atmospheric Sciences Texas A&M University T. Mauritsen and B. Stevens Max Planck Institute for Meteorology

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Page 1: A revision of the Earth’s energy balance framework - NASA · A revision of the Earth’s energy balance framework A. E. Dessler ... 5/17/2017 5:07:39 PM

A revision of the Earth’s energy balance framework

A. E. DesslerDept. of Atmospheric Sciences

Texas A&M University

T. Mauritsen and B. StevensMax Planck Institute for Meteorology

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abrupt 4xCO2 GFDL-CM3

Year

∆R∆T

s

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abrupt 4xCO2 GFDL-CM3

Year

∆R∆T

s

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abrupt 4xCO2 GFDL-CM3

Year

∆R∆T

s

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abrupt 4xCO2 GFDL-CM3

Year

∆F∆R∆T

s

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abrupt 4xCO2 GFDL-CM3

∆Ts

∆R

Year

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Year

abrupt 4xCO2 GFDL-CM3

∆R∆T

s

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Year

abrupt 4xCO2 GFDL-CM3

∆R

∆R = ∆F + λ ∆Ts

∆Ts

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∆R = ∆F + λ ∆Ts = 0

At equilibrium:

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∆R = ∆F + λ ∆Ts

∆Ts = -∆F/λ

= 0

At equilibrium:

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∆R = ∆F + λ ∆Ts

∆Ts = -∆F/λ

= 0

At equilibrium:

∆T2xCO2 = -∆F2xCO2/λ = ECS

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∆R = ∆F + λ ∆Ts

∆Ts = -∆F/λ

= 0

At equilibrium:

∆T2xCO2 = -∆F2xCO2/λ = ECS

Q: is this the right way to describe our planet’s energy balance?

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∆R = ∆F + λ ∆Ts

∆Ts = -∆F/λ

= 0

At equilibrium:

∆T2xCO2 = -∆F2xCO2/λ = ECS

Q: is this the right way to describe our planet’s energy balance?

Q: is the response of the TOA flux linear in global avg. surface

temperature?

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6

satellite obs. record (2000-2016)

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7

satellite obs. record (2000-2016)

∆R = ΔF + λ ΔTS

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7

satellite obs. record (2000-2016)

∆R = ΔF + λ ΔTS CERES

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7

satellite obs. record (2000-2016)

∆R = ΔF + λ ΔTS obs.CERES

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7

satellite obs. record (2000-2016)

∆R = ΔF + λ ΔTS obs.CERES

small

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∆R

∆Ts

∆R = ΔF + λ ΔTS

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∆R

∆Ts

∆R = ΔF + λ ΔTS

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∆R

∆Ts

Slope = λ (W/m2/K)

∆R = ΔF + λ ΔTS

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CER

ES E

d. 4

, EBA

F

ERAi

Global, monthly avg., detrended, 3/2000-9/2016

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CER

ES E

d. 4

, EBA

F

ERAi

Global, monthly avg., detrended, 3/2000-9/2016

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CER

ES E

d. 4

, EBA

F

ERAi

Global, monthly avg., 3/2000-9/2016Lesson: λ∆T is not a very good parameterization for ∆R (for

interannual variability)

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CER

ES E

d. 4

, EBA

F

ERAi

Global, monthly avg., 3/2000-9/2016Lesson: λ∆T is not a very good parameterization for ∆R (for

interannual variability)

Should not be surprising: 90% of TOA LW radiation emitted

by atmosphere, not surface

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12

Derive ECS & λ from 20th century record

∆R = ΔF + λ ΔTS

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12

Derive ECS & λ from 20th century record

∆R = ΔF + λ ΔTS obs.

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12

Derive ECS & λ from 20th century record

∆R = ΔF + λ ΔTS climate model

obs.

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12

Derive ECS & λ from 20th century record

∆R = ΔF + λ ΔTS climate model

obs.OHC

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13

∆R = ΔF + λ ΔTS climate model

obs.

λ ≈ -2 W/m2/K ECS ≈ 1.5-2.0 K

OHC

Derive λ from 20th century record

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13

∆R = ΔF + λ ΔTS climate model

obs.

λ ≈ -2 W/m2/K ECS ≈ 1.5-2.0 K

OHC

This anchors the low end of the IPCC's ECS range to 1.5 K

Derive λ from 20th century record

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14

∆R = ΔF + λ ΔTS

ΔF obs.

ΔR ΔTS

modelssame same same

λ ≈ -2 W/m^2 λ ≈ -1.3ECS < 2 K ECS 2-4.5 K

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14

∆R = ΔF + λ ΔTS

ΔF obs.

ΔR ΔTS

modelssame same same

λ ≈ -2 W/m^2 λ ≈ -1.3ECS < 2 K ECS 2-4.5 K

Page 34: A revision of the Earth’s energy balance framework - NASA · A revision of the Earth’s energy balance framework A. E. Dessler ... 5/17/2017 5:07:39 PM

Perfect model experiment

• 100-member MPI-ESM1.1 ensemble – model producing output for CMIP6

• 1850-2005; identical historical forcing • only difference is the initial conditions

15

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16

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17

For each ensemble member …

∆R = ΔF + λ ΔT

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17

For each ensemble member …

∆R = ΔF + λ ΔT

solve for this

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18

λ = ∆(R-F)/∆Ts W/m2/K

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18

λ = ∆(R-F)/∆Ts W/m2/K

internal variability

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19

λ = ∆(R-F)/∆Ts ECS = -∆F2xCO2/λ

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19

λ = ∆(R-F)/∆Ts ECS = -∆F2xCO2/λ

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19

λ = ∆(R-F)/∆Ts ECS = -∆F2xCO2/λ

We only have one realization of the 20th century, so there’s no guarantee that λ and ECS based on these

calculations are good estimates

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20

revised framework

∆R = ΔF + Θ ΔTA

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20

revised framework

∆R = ΔF + Θ ΔTA 500-hPa tropical

temperatures

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20

revised framework

∆R = ΔF + Θ ΔTA 500-hPa tropical

temperatures

following Trenberth, Murphy, Spencer

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20

revised framework

∆R = ΔF + Θ ΔTA 500-hPa tropical

temperaturesConverts change

in TA to flux; replaces λ

following Trenberth, Murphy, Spencer

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CERES Ed. 4 TOA fluxes & ERA-interim temperatures monthly avg. detrended anomalies

Ts = global avg. surface temperature TA = tropical avg. 500-hPa temperature

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22

λ = ∆(R-F)/∆TSΘ = ∆(R-F)/∆TA

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22

λ = ∆(R-F)/∆TSΘ = ∆(R-F)/∆TA

confirmed in CMIP5 control runs

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23

∆R = ΔF + Θ ΔTA

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• Can we use our new framework to better predict ECS?

23

∆R = ΔF + Θ ΔTA

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• Can we use our new framework to better predict ECS?

• Use measurement of Θcontrol from CERES to constrain ECS

23

∆R = ΔF + Θ ΔTA

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• Can we use our new framework to better predict ECS?

• Use measurement of Θcontrol from CERES to constrain ECS

• In CMIP5 ensemble, Θcontrol ≈ Θabrupt4xCO2

25

∆R = ΔF + Θ ΔTA

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3.45 K

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3.45 K

13 of 15

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3.45 K3 of 13

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3.45 K

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3.45 K

ECS < 3.5 K

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• the conventional energy balance framework has problems — TOA flux is not strongly related to surface temperature

• creates problems inferring ECS from historical data

• new framework using atmospheric temperature: ECS < 3.5 K

31

Conclusions

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backup slides

32

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CERES ∆R at each latitude vs. ∆Ts at that same latitude detrended monthly avg. anomalies

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global vs. tropical T500

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35

20th century obs. record

∆R = ΔF + λ ΔT

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35

20th century obs. record

∆R = ΔF + λ ΔT based on fixed SST runs

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35

20th century obs. record

∆R = ΔF + λ ΔT based on fixed SST runs

ensemble

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35

20th century obs. record

∆R = ΔF + λ ΔT based on fixed SST runs

ensembleensemble

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∆T

∆R

CMIP5 control runs (NorESM1-M)

months

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∆T

∆R

CMIP5 control runs (NorESM1-M)

months

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∆T

∆R

CMIP5 control runs (NorESM1-M)

months

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∆T

∆R

CMIP5 control runs (NorESM1-M)

months

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∆T

∆R

CMIP5 control runs (NorESM1-M)

months

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∆T

∆R

CMIP5 control runs (NorESM1-M)

months

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37

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38

CCSM4 CMIP5 control run

λ = ∆(R-F)/∆Ts

Θ = ∆(R-F)/∆T500t

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39

CMIP5 control runs

5-95% percentile range

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2.4 K

3.45 K

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2.4 K

3.45 K

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2.4 K

3.45 K

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2.4 K

3.45 K 3 of 13 models

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2.4 K

3.45 K

11 of 11 models