Micrometeorological Methods Used to Measure Greenhouse Gas Fluxes: The Challenges Associated with Them, at the Local to Global Scales Dennis Baldocchi University of California, Berkeley JASON GHG Emissions Monitoring Summer Study (June 16-18, 2010) La Jolla, CA Methods To Assess Terrestrial Carbon Budgets at Landscape to Continental Scales, and Across Multiple Time Scales GCM Inversion Modeling Remote Sensing/ MODIS Physiological Measurements/ Manipulation Expts. Eddy Flux Measurements/ FLUXNET Forest/Biomass Inventories Biogeochemical/ Ecosystem Dynamics Modeling From point to globe via integration with remote sensing (and gridded metorology) century forest inventory plot Forest/soil inventories decade Temporal scale year month Landsurface remote sensing Eddy covariance towers week tall tower observatories remote sensing of CO2 day hour local 0.1 1 plot/site From: Markus Reichstein, MPI 10 100 1000 10 000 global Countries EU Spatial scale [km] Challenges in Measuring Greenhouse Gas Fluxes • Measuring/Interpreting greenhouse gas flux in a quasicontinuous manner for days, years and decades • Measuring/Interpreting fluxes over Patchy, Microbiallymediated Sources (e.g. CH4, N2O) • Measuring/Interpreting fluxes of Temporally Intermittent Sources (CH4, N2O, O3, C5H8) • Measuring/Interpreting fluxes over Complex Terrain • Developing New Sensors for Routine Application of Eddy Covariance, or Micrometeorological Theory, for trace gas Flux measurements and their isotopes (CH4, N2O,13CO2, C18O2) • Measuring fluxes of greenhouse gases in Remote Areas without ac line power Flux Methods Appropriate for Slower Sensors, e.g. FTIR F w' c' w (c up c dn ) • Relaxed Eddy Accumulation • Modified Gradient Approach • Integrated Profile • Disjunct Sampling z z c z Fc ~ Fs sz 1 F u( c background )dz x0 Eddy Covariance • Direct Measure of the Trace Gas Flux Density between the atmosphere and biosphere, mole m-2 s-1 • Introduces No Sampling artifacts, like chambers • Quasi-continuous • Integrative of a Broad Area, 100s m2 • In situ ESPM 228 Adv Topics Micromet & Biomet Eddy Covariance, Flux Density: mol m-2 s-1 or J m-2 s-1 F a ws ~ a w ' s ' c mc pc s a ma Pa ESPM 228 Adv Topics Micromet & Biomet Eddy Covariance Tower Sonic Anemometer, CO2/H2O IRGA, inlet for CH4 Tunable diode laser spectrometer & Meteorological Sensors 24 Hour Time Series of 10 Hz Data, Vertical Velocity (w) and Methane (CH4) Concentration 4 W m/s 2 0 -2 -4 0 1 2 3 4 5 6 7 8 9 5 x 10 5 4.5 CH 4 ppm 4 3.5 D164, 2008 3 2.5 2 1.5 0 1 2 3 4 5 seconds Sherman Island, CA: data of Detto and Baldocchi 6 7 8 9 5 x 10 Non-Dispersive Infrared Spectrometer, CO2 and H2O Open-path , 12.5 cm Low Power, 10 W Low noise, CO2: 0.16 ppm; H2O: 0.0047 ppth Low drift, stable calibration Low temperature sensitivity: 0.02%/degree C LI 7500 Measuring Methane with Off-Axis Infrared Laser Spectrometer Closed path Moderate Cell Volume, 400 cc Long path length, kilometers High power Use: Sensor, 80 W Pump, 1000 W; 30-50 lpm Low noise: 1 ppb at 1 Hz Stable Calibration Los Gatos Research LI-7700 Methane Sensor, variant of frequency modulation spectroscopy Open path, 0.5 m Short optical path length, 30 m Low Power Use: 8 W, no pump Moderate Noise: 5 ppb at 10 Hz Stable Calibration Power Spectrum defines the Frequencies to be Sampled Power Spectrum w' w' S ww ( )d 0 Co-Spectrum F w' c' S wc ( )d 0 ESPM 228 Adv Topics Micromet & Biomet Signal Attenuation: The Role of Filtering Functions and Spectra • High and Low-pass filtering via Mean Removal – Sampling Rate (1-10Hz) and Averaging Duration (30-60 min) • Digital sampling and Aliasing • Sensor response time • Sensor Attenuation of signal – Tubing length and Volumetric Flow Rate – Sensor Line or Volume averaging • Sensor separation – Lag and Lead times between w and c ESPM 228 Adv Topics Micromet & Biomet Comparing Co-spectra of open-path CO2 & H2O sensor and closed-path CH4 sensor Co-Spectra are More Forgiving of Inadequate Sensor Performance than Power Spectra Because there is little w-c correlation in the inertial subrange M.Detto and D. Baldocchi Co-Spectra is a Function of Atmospheric Stability: Shifts to Shorter Wavelengths under Stable Conditions Shifts to Longer Wavelengths under Unstable Conditions Detto, Baldocchi and Katul, Boundary Layer Meteorology, accepted Zero-Flux Detection Limit, Detecting Signal from Noise F w ' c ' rwc w c rwc ~ 0.5 ch4 ~ 0.84 ppb co2 ~ 0.11 ppm Methane Sensor 0.1 0.2 0.3 0.4 0.5 Mean: 1897.4277 StdDev: 0.8411 Std Err 0.0219 1910 w m/s U* m/s Methane Lab Calibration 1920 1900 1890 1880 260 280 300 320 340 360 380 400 Time ESPM 228 Adv Topics Micromet & Biomet Fmin, CH4 Fmin, CO2 nmol m-2 s-1 mmol m-2 s-1 0.125 2.1 0.275 0.25 4.2 0.55 0.375 6.3 0.825 0.5 8.4 1.1 0.625 10.5 1.375 Flux Detection Limit, v2 Based on 95% CI that the Correlation between W and C that is non-zero 0.035 mmol m-2 s-1, 0.31 mmol m-2 s-1 and 3.78 nmol m-2 s-1 for water vapour, carbon dioxide and methane flux, Detto et al, in prep Most Sensors Measure Mole Density, Not Mixing Ratio Formal Definition of Eddy Covariance, V2 F a ws a w' s' w c w' c ' w c ESPM 228 Adv Topics Micromet & Biomet Webb, Pearman, Leuning Algorithm: ‘Correction’ for Density Fluctuations when using Open-Path Sensors ma c v ma c ' Fc w' c ' w' v (1 ) w' T ' mv a a mv T ESPM 228 Adv Topics Micromet & Biomet Raw <w’c’> signal, without density ‘corrections’, will infer Carbon Uptake when the system is Dead and Respiring Fwpl <w'c'> dead annual grassland 10 F (mmol m-2 s-1) 5 0 -5 -10 -15 -20 180 181 182 183 Day ESPM 228 Adv Topics Micromet & Biomet 184 185 methane correction term for <wt>, nmol m-2 s-1 methane correction term for water vapor, nmol m-2 s-1 Density ‘Corrections’ Are More Severe for CH4 and N2O: This Imposes a Need for Accurate and Concurrent Flux Measurements of H and LE 20 18 16 14 12 10 8 6 4 2 0 0 2 4 6 -2 -1 wq mmol m s 8 10 120 100 80 60 40 20 0 0 0.1 0.2 0.3 -1 wt K m s 0.4 Annual Time Scale, Open vs Closed sensors Hanslwanter et al 2009 AgForMet ESPM 228 Adv Topics Micromet & Biomet Towards Annual Sums Accounting for Systematic and Random Bias Errors • Advection/Flux Divergence • U* correction for lack of adequate turbulent mixing at night • QA/QC for Improper Sensor Performance – Calibration drift (slope and intercept), spikes/noise, a/d off-range – Signal Filtering • Software Processing Errors • Lack of Fetch/Spatial Biases – Sorting by Appropriate Flux Footprint • Change in Storage • Gaps and Gap-Filling ESPM 228 Adv Topic Micromet & Biomet Systematic and Random Errors 3 signal random error 2 1 0 f(t) -1 -2 -3 0 1 2 3 4 5 6 7 time 2.0 1.5 signal bias error 1.0 0.5 f(t) 0.0 -0.5 -1.0 -1.5 0 1 2 3 4 5 6 7 time 1.5 1.0 0.5 0.0 f(t) -0.5 signal systematic bias -1.0 -1.5 0 1 2 3 4 5 time ESPM 228 Adv Topic Micromet & Biomet 6 7 Random Errors Diminish as We Measure Fluxes Annually and Increase the Sample Size, n Oak Ridge, TN Temperate Deciduous Forest 1997 15 10 5 Tall Vegetation, Undulating Terrain -5 -10 -15 -20 -25 -30 -35 -40 100 150 200 250 300 350 Vaira Grassland 2001 Day-Hour 15 10 5 -1 50 0 -2 0 Fc (mmol m s ) Fwpl (mmol m-2 s-1) 0 Short Vegetation, Flat Terrain -5 -10 -15 -20 -25 0 50 100 150 200 Day/Hour 250 300 350 Systematic Biases and Flux Resolution: A Perspective • FCO2: +/- 0.3 mmol m-2 s-1 => +/- 113 gC m-2 y-1 • 1 sheet of Computer paper 1 m by 1 m: ~70 gC m-2 y-1 • Net Global Land Source/Sink of 1PgC (1015g y-1): 6.7 gC m-2 y-1 The Real World is Not Kansas, which is Flatter than a Pancake Eddy Covariance in the Real World Cloud Cloud ESPM 228 Adv Topics Micromet & Biomet Diagnosis of the Conservation Equation for C for Turbulent Flow u j ' c ' dc c c c c u ' c ' v ' c ' w ' c ' u v w dt t x y z x j x y z I III II I: Time Rate of Change II: Advection III: Flux Divergence ESPM 228 Adv Topics Micromet & Biomet Daytime and Nightime Footprints over an Ideal, Flat Paddock F 0 z F F dz Const z Detto et al. Boundary Layer Meteorology, conditionally accepted Estimating Flux Uncertainties: Two Towers over Rice Detto, Anderson, Verfaillie, Baldocchi, unpublished Examine Flux Divergence Detto, Baldocchi and Katul, Boundary Layer Meteorology, conditionally accepted Underestimating C efflux at Night, Under Tall Forests, in Undulating Terrain 10 5 -1 -2 mmol m s CO2 Flux Density 0 -5 -10 -15 -20 -25 0 4 8 12 16 20 24 time (hours) Ne: measured (-4.84 gC m-2 day-1) Ne: computed (-5.09 gC m-2 day-1) Fwpl+Storage: measured (-5.96 gC m-2 day-1) Fwpl: measured (-6.12 gC m-2 day-1) Baldocchi et al., 2000 BLM Losses of CO2 Flux at Night: u* correction Wheat, Columbia River Valley, Oregon 8 Canopy Respiration 8 to 13 C 7 r ² 0.325 Fco2 (mmol m-2 s-1) 6 5 4 3 2 1 0 0.0 0.2 0.4 0.6 u* (m s-1) ESPM 228 Adv Topic Micromet & Biomet 0.8 1.0 Systematic Biases are an Artifact of Low Nocturnal Wind Velocity Friction Velocity, m/s Annual Sums comparing Open and Closed Path Irgas Hanslwanter et al 2009 AgForMet ESPM 228 Adv Topics Micromet & Biomet Biometric and Eddy Covariance C Balances Converge after Multiple Years Gough et al. 2008, AgForMet Contrary Evidence from Personal Experience: Crops, Grasslands and Forests Boreas 1994 Hourly averages 600 800 wheat 500 700 r2=0.98 slope=1.05 Old Jack Pine r2=0.93 slope=0.93 LE+H+S+G (W m-2) 600 H+LE (W m-2) 400 300 200 500 400 300 200 100 100 0 -100 -100 0 -100 -100 0 100 200 300 Rn-G (W m-2) 400 500 300 400 500 600 700 800 400 Coefficients: b[0] 3.474 300 b[1] 1.005 r² coefficients: b[0] 5.55 b[1] 0.94 r ² 0.926 0.923 LE+H+G E + H + G + S + Ps (W m ) 200 Vaira Grassland, D296-366, 2000 800 -2 100 Rn (W m-2) Temperate Deciduous Forest 600 0 600 400 200 100 200 0 0 0 200 400 600 800 -100 -100 0 100 200 -2 -2 Rnet (W m ) Rnet (W m ) 300 400 Many Studies Don’t Consider Heat Storage of Forests Well, or at All, and Close Energy Balance when they Do Lindroth et al 2010 Biogeoscience Haverd et al 2007 AgForMet ESPM 228 Adv Topic Micromet & Biomet FLUXNET: From Sea to Shining Sea 500+ Sites, circa 2009 Limits and Criteria for Network Design for Treaty Verification • Can We Statistically-Sample or Augment Regional, Continental and Global Scale C Budgets with a Sparse Network of Flux Towers? • If Yes: – How Many Towers are Enough? – Where Should the Towers Be? – How Good is Good Enough with regards to Fluxes? – How Long Should We Collect Data? How many Towers are needed to estimate mean NEE, GPP and assess Interannual Variability, at the Global Scale? Green Plants Abhor a Vacuum, Most Use C3 Photosynthesis, so we May Not need to be Everywhere, All of the Time We Need about 75 towers to produce Robust and Invariant Statistics Probability Distribution of Published NEE Measurements, Integrated Annually 0.07 0.06 0.05 mean: -182.9 gC m-2 y-1 std dev: 269.5 n: 506 p(x) 0.04 0.03 0.02 0.01 0.00 -1500 -1000 -500 0 FN (gC m-2 y-1) Baldocchi, Austral J Botany, 2008 500 1000 1500 Interannual Variability of the Statistics of NEE is Small across a sub-network of 75 Sites Mean NEE Ranges between -220 to -243 gC m-2 y-1 Standard Deviation Ranges between 35.2 and 39.9 gC m-2 y-1 0.25 FLUXNET Network, 75 sites 2002: -220 +/- 35.2 gC m-2 y-1 2003: -238 +/- 39.9 2004: -243 +/- 39.7 2005: -237 +/- 38.7 0.20 p(NEE) 0.15 0.10 0.05 0.00 -1000 -800 -600 -400 -200 0 NEE (gC m-2 y-1) 200 400 600 Interannual Variability in GPP is small, too, across the Global Network (1103 to 1162 gC m-2 y-1) 2002: 1117 +/- 74.0gC m 2003: 1103 +/- 67.8 2004: 1162 +/- 77.0 2005: 1133 +/- 70.1 -2 -1 y 0.25 FLUXNET Network, 75 sites p(GPP) 0.20 0.15 0.10 0.05 0.00 0 500 1000 1500 2000 2500 3000 3500 GPP (gC m-2 y-1) Assuming Global Arable Land area is 110 106 km2, Mean Global GPP ranges between 121.3 and 127.8 PgC/y Precision is about +/- 7 PgC/y Ecosystem Respiration Scales Tightly with Ecosystem Photosynthesis, But Is with Offset by Disturbance 4000 Undisturbed Disturbed by Logging, Fire, Drainage, Mowing 3500 FR (gC m-2 y-1) 3000 2500 2000 1500 1000 500 0 0 500 1000 1500 2000 2500 FA (gC m-2 y-1) Baldocchi, Austral J Botany 2008 3000 3500 4000 Net Carbon Exchange is a Function of Time Since Disturbance Conifer Forests, Canada and Pacific Northwest 1000 800 FN (gC m-2 y-1) 600 400 200 0 -200 -400 -600 1 10 100 Stand Age After Disturbance Baldocchi, Austral J Botany, 2008 1000 C Fluxes May Vary Interannual on 7 to 10 year Time Scales Walker Branch Watershed, TN: 1981-2001 CANOAK 1 year 130 days nSnee/nee 0.1 0.01 7 years 0.001 0.0001 0.0001 0.001 0.01 Frequency (1/day) 0.1 1 Upscale NEP, Globally, Explicitly 1. Compute GPP = f(T, ppt) 2. Compute Reco = f(GPP, Disturbance) 3. Compute NEP = GPP-Reco Leith-Reichstein Model GPP min f MAT , g P 1 e a1 a2 15C 1 e k P min GPP15C , GPP1000mm a1 a2 MAT k 1000mm 1 e 1 e 4000 Undisturbed Disturbed by Logging, Fire, Drainage, Mowing 3500 FLUXNET Synthesis Baldocchi, 2008, Aust J Botany FR (gC m-2 y-1) 3000 2500 2000 Reco = 101 + 0.7468 * GPP 1500 1000 Reco, disturbed= 434.99 + 0.922 * GPP 500 0 0 500 1000 1500 2000 2500 FA (gC m-2 y-1) 3000 3500 4000 <NEE> = -222 gC m-2 y-1 This Flux Density Matches FLUXNET (-225) well, but S NEE = -31 PgC/y!! Implies too Large NEE (|-700 gC m-2 y-1| Fluxes in Tropics Ignores C losses from Disturbance and Land Use Change Explicit Climate-Based Upscaling Under Represents Disturbance Effects FLUXNET Database 0.14 0.12 0.10 FLUXNET Global Map pdf 0.08 0.06 FLUXNET Under Samples Tropics 0.04 0.02 0.00 -1400 -1200 -1000 -800 -600 -400 -200 0 NEE (gC m-2 y-1) Statistically Sampling and Climate Upscaling Agree <NEE: FLUXNET> = -225 +/- 164 gC m-2 y-1 <NEE 0% dist: sinusoidal> = -222 gC m-2 y-1 200 400 600 To Balance Carbon Fluxes infers that Disturbance Effects May Be Greater than Presumed <NEE> = -4.5 gC m-2 y-1 S NEE = -1.58 PgC/y UpScaling Tower Based C Fluxes with Remote Sensing LIDAR derived map of Tree location and Height Hemispherical Camera Web Camera Upward Looking Camera Annual Grassland, 2004-2005 1.0 Reflectance 0.8 Oct 13, 2004 Oct 27, 2004 Nov 11, 2004 Jan 5, 2005 Feb 2, 2005 Apr 1, 2005 Mar 9, 2005 May 11, 2005 Dec 29, 2005 0.6 0.4 0.2 0.0 400 500 600 700 800 Wavelength (nm) Falk, Ma and Baldocchi, unpublished ESPM 111 Ecosystem Ecology 900 1000 Ground Based, Time Series of Hyper-Spectral Reflectance Measurements, in Conjunction with Flux Measurements Can be Used to Design Future Satellites Remote Sensing of NPP: Up and down PAR, LED, Pyranometer, 4 band Net Radiometer LED-based sensors are Cheap, Easy to Replicate and Can be Designed for a Number of Spectral Bands Spectrally-Selective Vegetation Indices Track Seasonality of C Fluxes Well Ryu et al. Agricultural and Forest Meteorology, in review Vegetation Indices can be Used to Predict GPP with Light Use Efficiency Models Ryu et al. Agricultural and Forest Meteorology, in review UpScaling of FluxNetworks What We can Do: Is Precision Good Enough for Treaties? Xiao et al 2010, Global Change Biology Map of Gross Primary Productivity Derived from Regression Tree Algorithms Derived from Flux Network, Satellite Remote Sensing and Climate Data Xiao et al 2010, Global Change Biology Xiao et al 2010, Global Change Biology Net Ecosystem C Exchange spring summer autumn Xiao et al. 2008, AgForMet winter Upscale GPP and NEE to the Biome Scale area-averaged fluxes of NEE and GPP were -150 and 932 gC m-2 y-1 net and gross carbon fluxes equal -8.6 and 53.8 TgC y-1 Jingfeng Xiao and D Baldocchi Take-Home Message for Application of Eddy Covariance Method under Non-Ideal Conditions •Routine Flux Measurements Must Comply with Governing Principles of Conservation Equation •Design Experiment that measures Flux Divergence and Storage, in addition to Covariance •Networks need more Sites in Tropics and Distinguish C3/C4 crops •Networks need Sites that Cover a Range of Disturbance History •Network of Flux Towers, in conjunction with Remote Sensing, Climate Networks and Machine Learning Algorithms has Potential to Produce Carbon Flux Maps for Carbon Monitoring for Treaty, with Caveats and Accepted Errors Additional Background Material Sampling Error with Two Towers Hollinger et al GCB, 2004 Gap-Filling Inter-comparison Bias Errors Moffat et al., 2007, AgForMet ESPM 228 Adv Topic Micromet & Biomet Root Mean Square Errors with Different Gap Filling Methods Moffat et al., 2007, AgForMet ESPM 228 Adv Topic Micromet & Biomet