Interannual variability of top-ofatmosphere. CERES instruments

Similar documents
Variability in Global Top-of-Atmosphere Shortwave Radiation Between 2000 And 2005

Influence of Clouds and Aerosols on the Earth s Radiation Budget Using Clouds and the Earth s Radiant Energy System (CERES) Measurements

Lecture 3. Background materials. Planetary radiative equilibrium TOA outgoing radiation = TOA incoming radiation Figure 3.1

Seeking a consistent view of energy and water flows through the climate system

Constraints on the Interannual Variation of Global and Regional Topof-Atmosphere. Inferred from MISR Measurements. Roger Davies

Solar Insolation and Earth Radiation Budget Measurements

Radiation balance of the Earth. 6. Earth radiation balance under present day conditions. Top of Atmosphere (TOA) Radiation balance

and Atmospheric Science, University of Miami, 4600 Rickenbacker Causeway, Miami, FL 33149, USA.

P1.30 THE ANNUAL CYCLE OF EARTH RADIATION BUDGET FROM CLOUDS AND THE EARTH S RADIANT ENERGY SYSTEM (CERES) DATA

Changes in Earth s Albedo Measured by satellite

History of Earth Radiation Budget Measurements With results from a recent assessment

Seasonal and interannual variations of top-of-atmosphere irradiance and cloud cover over polar regions derived from the CERES data set

CERES_EBAF-Surface_Ed2.7 Data Quality Summary (June 7, 2013)

The Arctic Energy Budget

9.4. The newly released 5-year Terra-based monthly CERES radiative flux and cloud product. David R. Doelling, D. F. Keyes AS&M, Inc.

Climate Feedbacks from ERBE Data

Radiation in climate models.

ATMOS 5140 Lecture 1 Chapter 1

Introduction to Climate ~ Part I ~

The effect of ocean mixed layer depth on climate in slab ocean aquaplanet ABSTRACT

Extratropical and Polar Cloud Systems

Understanding the Greenhouse Effect

T. Dale Bess 1 and Takmeng Wong Atmospheric Sciences Division Langley Research Center, NASA Hampton, VA G. Louis Smith

Deducing Earth s Global Energy Flows from a Simple Greenhouse Model

Impact of Sun-Synchronous Diurnal Sampling on Tropical TOA Flux Interannual Variability and Trends

Advances in Understanding Top-of-Atmosphere Radiation Variability from Satellite Observations

Earth s Energy Balance and the Atmosphere

Climate Change: Moonshine, Millions of Models, & Billions of Data New Ways to Sort Fact from Fiction

The Spectral Radiative Effects of Inhomogeneous Clouds and Aerosols

SATELLITE OBSERVATIONS OF CLOUD RADIATIVE FORCING FOR THE AFRICAN TROPICAL CONVECTIVE REGION

The Energy Balance Model

A perturbed physics ensemble climate modeling. requirements of energy and water cycle. Yong Hu and Bruce Wielicki

Global Energy and Water Budgets

1) The energy balance at the TOA is: 4 (1 α) = σt (1 0.3) = ( ) 4. (1 α) 4σ = ( S 0 = 255 T 1

Friday 8 September, :00-4:00 Class#05

Interpretation of Polar-orbiting Satellite Observations. Atmospheric Instrumentation

Earth s Radiation Budget & Climate

The flow of Energy through the Earth s Climate System: Land and Ocean Exchanges

On the Satellite Determination of Multilayered Multiphase Cloud Properties. Science Systems and Applications, Inc., Hampton, Virginia 2

J. Xing et al. Correspondence to: J. Xing

Lecture 8. Monsoons and the seasonal variation of tropical circulation and rainfall

Sensitivity of climate forcing and response to dust optical properties in an idealized model

Can we measure from satellites the cloud effects on the atmospheric radiation budget?

An Observational Study of the Relationship between Cloud, Aerosol and Meteorology in Marine Stratus Regions

Surface Radiation Budget from ARM Satellite Retrievals

5. General Circulation Models

ATOC 5051 INTRODUCTION TO PHYSICAL OCEANOGRAPHY. Lecture 19. Learning objectives: develop a physical understanding of ocean thermodynamic processes

How good are our models?

Saharan Dust Induced Radiation-Cloud-Precipitation-Dynamics Interactions

9/5/16. Section 3-4: Radiation, Energy, Climate. Common Forms of Energy Transfer in Climate. Electromagnetic radiation.

GEO1010 tirsdag

Connection between NAO/AO, surface climate over Northern Eurasia: snow cover force - possible mechanism.

Electromagnetic Radiation. Radiation and the Planetary Energy Balance. Electromagnetic Spectrum of the Sun

Comparison of MISR and CERES top-of-atmosphere albedo

Arctic Climate Change. Glen Lesins Department of Physics and Atmospheric Science Dalhousie University Create Summer School, Alliston, July 2013

Dynamical balances and tropical stratospheric upwelling

Chapter 3- Energy Balance and Temperature

The effect of ocean mixed layer depth on climate in slab ocean aquaplanet experiments

- matter-energy interactions. - global radiation balance. Further Reading: Chapter 04 of the text book. Outline. - shortwave radiation balance

An Overview of the Radiation Budget in the Lower Atmosphere

Chapter 2 Solar and Infrared Radiation

Satellite-based estimate of global aerosol-cloud radiative forcing by marine warm clouds

3. Carbon Dioxide (CO 2 )

Next-generation angular distribution models for top-of-atmosphere radiative flux calculation from CERES instruments: validation

Understanding Climate Feedbacks Using Radiative Kernels

Patterns in the CERES Global Mean Data, Part 3

Clouds in the Climate System: Why is this such a difficult problem, and where do we go from here?

Southern Ocean albedo, inter hemispheric energy transports and the double ITCZ: global impacts of biases in a coupled model

Observational constraints on Arctic Ocean clouds and radiative fluxes during the early 21st century

Let s make a simple climate model for Earth.

Impact of the 2002 stratospheric warming in the southern hemisphere on the tropical cirrus clouds and convective activity

Lecture 2 Global and Zonal-mean Energy Balance

The effect of ocean mixed layer depth on climate in slab ocean aquaplanet experiments

Radiation in the atmosphere

Steady Flow: rad conv. where. E c T gz L q 2. p v 2 V. Integrate from surface to top of atmosphere: rad TOA rad conv surface

Radiation, Sensible Heat Flux and Evapotranspiration

Monday 9 September, :30-11:30 Class#03

P1.6 DIURNAL CYCLES OF THE SURFACE RADIATION BUDGET DATA SET

On the use of satellite remote sensing to determine direct aerosol radiative effect over land : A case study over China

APPLICATIONS WITH METEOROLOGICAL SATELLITES. W. Paul Menzel. Office of Research and Applications NOAA/NESDIS University of Wisconsin Madison, WI

Variability in clear-sky longwave radiative cooling of the atmosphere

Characteristics of Global Precipitable Water Revealed by COSMIC Measurements

Earth Systems Science Chapter 3

Patterns in the CERES Global Mean Data, Part 3. Cloud Area Fraction, Atmospheric Energy Budgets, DLR Update. Miklos Zagoni

On assessing temporal variability and trends of coupled arctic energy budgets. Michael Mayer Leo Haimberger

Lecture 11: Meridonal structure of the atmosphere

Extreme, transient Moisture Transport in the high-latitude North Atlantic sector and Impacts on Sea-ice concentration:

Steven Feldstein. The link between tropical convection and the Arctic warming on intraseaonal and interdecadal time scales

The Influence of Obliquity on Quaternary Climate

How Accurate is the GFDL GCM Radiation Code? David Paynter,

The Earth Climate Hyperspectral Observatory: Advances in Climate Change Detection, Attribution, and Remote Sensing

Saharan Dust Longwave Radiative Forcing using GERB and SEVIRI

Remote Sensing Applications for Land/Atmosphere: Earth Radiation Balance

Global Climate Change

Clouds, Haze, and Climate Change

Arctic Clouds and Radiation Part 2

Assessing the impact of Arctic sea ice variability on Greenland Ice Sheet surface mass and energy exchange

Atmospheric circulation analysis for seasonal forecasting

May 3, :41 AOGS - AS 9in x 6in b951-v16-ch13 LAND SURFACE ENERGY BUDGET OVER THE TIBETAN PLATEAU BASED ON SATELLITE REMOTE SENSING DATA

SUPPLEMENTARY INFORMATION

Transcription:

Interannual variability of top-ofatmosphere albedo observed by CERES instruments Seiji Kato NASA Langley Research Center Hampton, VA SORCE Science team meeting, Sedona, Arizona, Sep. 13-16, 2011

TOA irradiance derived from CERES CERES: Clouds and Earth s Radiant Energy System Broadband instruments Measure shortwave, longwave (total-sw), and window radiances in a cross-track mode Currently, CERES instruments are on Terra and Aqua. Terra data start from March 2000 Aqua data start from July 2002 One instrument is on NPP Footprint size of instruments on Terra and Aqua is ~20 km TOA irradiance stability is 0.5 Wm -2 per decade More information is on http://ceres.larc.nasa.gov/

TOA SW Irradiance (W m -2 ) TOA irradiances are derived from angular distribution models Annual mean derived from 4-years of data (from March 2000 Feb. 2004)

TOA LW Irradiance (W m -2 ) Annual mean derived from 4-years of data (from March 2000 Feb. 2004)

Outline of this talk CERES instruments Top-of-atmosphere irradiance derived from CERES radiance measurements Surface irradiance computation De-seasonalized anomalies (defined in later slide) of irradiances Relationship between TOA albedo and cloud fraction de-seasonalized anomalies

Surface irradiances Surface shortwave and longwave irradiances are modeled by a radiative transfer model Inputs Temperature and humidity: Reanalysis Cloud and aerosol properties: MODIS, Geostationary satellites Consistency check Comparison with CERES derived irradiance (TOA) Comparison with surface observations CloudSat, CALIPSO, AIRS

Surface downward and upward irradiance (March 2000) Temperature and humidity: Reanalysis Cloud and aerosol properties: MODIS Modeled irradiances with a 2-stream model

Zonal vertical heating rate profile (200807) Atmospheric absorption = (TOA down TOA up) (Surface down Surface up) Modeled heating rates at Aqua overpass time

Some definitions to analyze variability Deseasonalized anomalies ΔF (e.g. deviation from a monthly mean value) F F F F 1 n Investigate the variability of radiation budget n i 1 F i

Standard deviation of deseasonalized anomalies at TOA (March 2000 to Feb 2004) Standard deviations computed from 1 o X 1 o monthly anomalies

Standard deviation of NET (SW+LW) anomalies (March 2000 to Feb 2004) Thick high clouds: Negative SW anomalies and positive LW anomalies partially cancel Low clouds: LW anomalies are small compared to SW anomalies

Shortwave TOA Flux anomaly (Wm -2 ) TOA albedo anomalies over tropics are well correlated with cloud fraction anomalies MODIS cloud fraction anomaly Loeb et al. GRL 2007 Why are albedo variability and cloud fraction variability so small?

Correlation between TOA shortwave irradiance and cloud cover anomalies Correlation coefficients in polar regions are smaller

Global mean reflected shortwave and cloud fraction anomalies Cloud cover anomalies monthly Reflected Shortwave anomalies 12month average When anomalies are averaged, global mean interannual variability is small

TOA irradiance and cloud cover anomalies The annual and global mean TOA reflected shortwave is 96.7 W m -2, with maximum and minimum value of 97.1 and 96.4 W m -2. The difference between the maximum and minimum values is 0.8% of the mean value. The annual and global mean OLR is 239 W m -2, and the difference between maximum and minimum values is 0.3% of the mean value. The annual and global mean cloud cover is 61.7%, and the difference between maximum and minimum values is 0.2% of the mean value.

Questions Why is global mean interannual variability of albedo so small compared to its mean value? Or what prevents the albedo perturbation by clouds to intensify with time? Investigate the reason from atmospheric energy perspective

Net shortwave irradiance anomalies Tropics 30 N to 30 S From March 2000 Shortwave irradiance anomalies caused by clouds is predominately deposited to the surface

Regional variability Standard deviation of 1 1 anomalies Similar to TOA anomalies, large variability is due to ENSO

Regional variability (Longwave) Standard deviation of 1 1 anomalies Wm -2 Wm -2

Surface SW net versus LW net Correlation between Δ surface SW net and Δ surface LW net F SW net (sfc) c p w h e d T dt F L F s F net LW (sfc) c p w h e v T Energy deposited by shortwave anomalies are used for Surface temperature change Latent heat flux Sensible heat flux Longwave emission Horizontal advection by ocean currents Negative correlation More SW net gives Less LW net Where positive net Is downward net flux

Correlation coefficients between atmospheric net irradiance and cloud cover Atmospheric net irradiance (SW + LW, energy deposited to the atmosphere by radiation) anomalies is well correlated with cloud fraction anomalies, indicating A close connection between cloud fraction variability and atmospheric energy

Assumption Albedo (Insolation) Clouds Outgoing longwave radiation Meridional temperature gradient Large scale dynamics Assumption: Large-scale dynamics, which is driven by temperature gradient, controls global mean cloud cover i.e. If large scale dynamics is constant, cloud cover is also constant

Zonal temperature anomalies Zonal mean thermodynamic equation Separate zonal mean temperature into climatological mean and anomaly Assumptions: Vertical velocity anomalies = C T Horizontal temperature advection anomalies = Diabatic heating anomalies = T t D 2 a T J (t) c p T y 2 (a C) T D 2 y 2 T J' c p T T c T T T 0 e (a C D 2 )t e i y where a < 0, C <0, and D>0 Kato, J Climate, 2009

Atmospheric temperature vs. Cloud cover Correlation coefficient between 300 hpa 1000 hpa geopotential height difference and cloud cover

Cloud cover decorrelation time Month Derived from 48 months of CALIPSO and CloudSat data Decorrelation time = (1+Φ)/(1-Φ), where Φ is autocorrelation with 1 month lag

Summary Interannual variability of global mean albedo is 0.8% of the mean value and interannual variability of longwave is 0.3% of the mean value. A large part of albedo variability is caused by cloud cover variability. Proposed hypothesis Temperature anomalies caused by albedo variability is dumped by dynamics and longwave emission. The time scale of the decay is smaller than a year. As a consequence, temperature anomalies decay exponentially with time, which provides small interannual variability of temperature and cloud cover.

Back-ups

Standard Deviation (W m -2 ) Zonal variability Latitude ( o ) Latitude ( o ) Latitude ( o ) Solid line: Mean standard deviation of 1 X 1 region in a latitudinal zone Dashed line: Standard deviation of zonal anomalies

Cloud cover versus albedo Interannual variability of cloud cover is less than 1% of the mean value Regions with 0.8 or greater correlation coefficient are colored

Zonal atmospheric SW, LW NET and temperature variability Atmospheric SW, LW, and NET 300 hpa 1000 hpa thickness Temporal variability of zonal mean computed with 48 monthly zonal deseasonalized anomalies Temperature variability in polar regions is caused by dynamics variabilities

A large LW net or Upward longwave irradiance anomalies do not appear very often over ocean

Clear-sky, All-sky variability Open circles: Clear-sky Closed circles: All-sky

Correlation between TOA shortwave irradiance and cloud cover anomalies

Cloud fraction