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aircraft and tower eddy covariance flux measurements

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aircraft and tower eddy covariance flux measurements. B. Gioli (IBIMET CNR, Italy). SSOS- Summer School on Optical Sampling (7-13 July 2011, Trento, Italy). Layout. 1. TOWER FLUX MEASUREMENTS 2. AIRCRAFT FLUX MEASUREMENTS 3. FLUX MANIPULATION EXPERIMENT. - PowerPoint PPT Presentation
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aircraft and tower eddy covariance flux aircraft and tower eddy covariance flux measurements measurements SSOS- Summer School on Optical Sampling (7-13 July 2011, Trento, Italy) B. Gioli (IBIMET CNR, Italy)
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Page 1: aircraft and tower eddy covariance flux measurements

aircraft and tower eddy covariance flux aircraft and tower eddy covariance flux

measurementsmeasurements

SSOS- Summer School on Optical Sampling  (7-13 July 2011, Trento, Italy)

B. Gioli (IBIMET CNR, Italy)

Page 2: aircraft and tower eddy covariance flux measurements

1. TOWER FLUX MEASUREMENTS

2. AIRCRAFT FLUX MEASUREMENTS

3. FLUX MANIPULATION EXPERIMENT

SSOS- Summer School on Optical Sampling  (7-13 July 2011, Trento, Italy)

Layout

Page 3: aircraft and tower eddy covariance flux measurements

1. TOWER FLUX MEASUREMENTS

- principles of the eddy covariance micrometeorological tecnique;

- how to use turbulence to measure fluxes

-tecnique assumptions and limitations

SSOS- Summer School on Optical Sampling  (7-13 July 2011, Trento, Italy)

Page 4: aircraft and tower eddy covariance flux measurements

wind & turbulence

SSOS- Summer School on Optical Sampling  (7-13 July 2011, Trento, Italy)

Page 5: aircraft and tower eddy covariance flux measurements

wind & turbulence

SSOS- Summer School on Optical Sampling  (7-13 July 2011, Trento, Italy)

air motion is 3D and made by 'fluctuations'

Page 6: aircraft and tower eddy covariance flux measurements

+CO2+CO2 -CO2-CO2

surface exchange

CO2 sink surface

downdraft (w-) updraft (w+)

SSOS- Summer School on Optical Sampling  (7-13 July 2011, Trento, Italy)

Page 7: aircraft and tower eddy covariance flux measurements

c1, c1, w1w1

c2, c2, w2w2

surface exchange (one eddy)

CO2 sink surface

downdraft (w-) updraft (w+)

SSOS- Summer School on Optical Sampling  (7-13 July 2011, Trento, Italy)

Flux associated to one eddy = c1w1 + c2w2

Page 8: aircraft and tower eddy covariance flux measurements

Fluctuations of vertical wind and scalarsc’ = c - cw’ = w - w

+CO2+CO2 -CO2-CO2

CO2 sink surface

downdraft (w-) updraft (w+)

N

kkk ccww

NcwcwFlux

11

1),cov(''

surface exchange (general)

Page 9: aircraft and tower eddy covariance flux measurements

''

''

''

''

* wuu

qwE

wcH

cwNEE

p

Fluxes from a typical EC tower(at typically 30 min resolution)

Net Ecosystem Exchange

Sensible heat flux

Latent heat flux = evapotransp.

Momentum flux = friction velocity

SSOS- Summer School on Optical Sampling  (7-13 July 2011, Trento, Italy)

Page 10: aircraft and tower eddy covariance flux measurements

-30

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-5

0

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20 0 3 7 10

14

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21 0 4 7 11 14

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ora

flu

sso

di C

O2

[mic

rom

oli

m-2 s

ec-1

]

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19 0 5 10

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20 1 6 11 16

21 2 7 12

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ora del giorno

w m

-2 H LE

NEE

H, LE

SSOS- Summer School on Optical Sampling  (7-13 July 2011, Trento, Italy)

Page 11: aircraft and tower eddy covariance flux measurements

EC hypothesis

1. ~Flat terrain 2. Homogeneity

3. Stationarity4. 'enough' turbulence

SSOS- Summer School on Optical Sampling  (7-13 July 2011, Trento, Italy)

Sdz wt

dz ux

dz wz

dz

I II III IV V

h

ss

h

s

h

s

hm m m m

0 0 0 0 ' '

Page 12: aircraft and tower eddy covariance flux measurements

Technology: 3D wind (fast) measurement

SSOS- Summer School on Optical Sampling  (7-13 July 2011, Trento, Italy)

Page 13: aircraft and tower eddy covariance flux measurements

Technology: CO2 & H2O (fast) measurements

Open Path IRGA (Infra Red Gas Analyzer)

SSOS- Summer School on Optical Sampling  (7-13 July 2011, Trento, Italy)

Page 14: aircraft and tower eddy covariance flux measurements

Isola di PianosaIsola di Pianosa

InstallationsNorunda, SveziaNorunda, Svezia

SSOS- Summer School on Optical Sampling  (7-13 July 2011, Trento, Italy)

Page 15: aircraft and tower eddy covariance flux measurements

FluxNet

SSOS- Summer School on Optical Sampling  (7-13 July 2011, Trento, Italy)

Page 16: aircraft and tower eddy covariance flux measurements

Complicating factors: 1. frequency response:do we measure ALL the flux by eddy covariance ?

Rn = SW↓ +LW ↓ - SW↑ -LW↑ (net radiation)

H + LE + G = Rn

H: sensible heat flux (EC measured)

LE: latent heat flux = evapotranspiration (EC measured)

G = soil heat flux (measured)

SSOS- Summer School on Optical Sampling  (7-13 July 2011, Trento, Italy)

Vaccari et al 2003

Page 17: aircraft and tower eddy covariance flux measurements

Cospectra W-CO2 (Li7500)

-0.100

0.000

0.100

0.200

0.300

0.01 0.1 1 10 100

Frequency [Hz]

nS

(n)

cospectra of CO2 and W

high freq. ~ parts of a secondlow freq. ~ minutes

SSOS- Summer School on Optical Sampling  (7-13 July 2011, Trento, Italy)

Complicating factors: 1. frequency response:do we measure ALL the flux by eddy covariance ?

Page 18: aircraft and tower eddy covariance flux measurements

Complicating factors: 2. footprint estimation

where the measured flux comes from ?

SSOS- Summer School on Optical Sampling  (7-13 July 2011, Trento, Italy)

Footprint area = area contributing to the observed flux

Footprint area extends upwind the observation point, and is a function of:

• Atmospheric stability

• Wind speed and direction

• Surface roughness

Footprint area is estimated trough models (analytic, stochastic, lagrangian back-trajectory)

Page 19: aircraft and tower eddy covariance flux measurements

Complicating factors: 3. CO2 flux partioning

SSOS- Summer School on Optical Sampling  (7-13 July 2011, Trento, Italy)

• approaches exist to partition NEE into GPP and Reco, based on night time fluxes to dirve a respiration response to temperature and soil water content (Reichstein et al 2003)

NEE = GPP – Reco

NEE = Net Ecosystem ExchangeGPP = Gross Primary Productivity

Reco = Ecosystem respiration

-30

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11 14

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11 15

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22 1 5 8

12

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22 2 5

ora

flu

sso

di C

O2

[mic

rom

oli

m-

2 sec

-1]

Page 20: aircraft and tower eddy covariance flux measurements

2. AIRCRAFT FLUX 2. AIRCRAFT FLUX MEASUREMENTSMEASUREMENTS

SSOS- Summer School on Optical Sampling  (7-13 July 2011, Trento, Italy)

Page 21: aircraft and tower eddy covariance flux measurements

Sky Arrow ERA

Attitude GPS Net Radiation

PAR Radiation

Surface T

Dew Point T

Videocamera

Pressure Sphere

T Fast Response

T Low Response

Novatel GPS

IRGA

GPS

ElectronicsSwitch BOX

Page 22: aircraft and tower eddy covariance flux measurements

Mobile Flux Platform (MFP)Mobile Flux Platform (MFP)

Measurement of 3D winds @ 50 Hz

CO2, H2O, T fast sensors

SSOS- Summer School on Optical Sampling  (7-13 July 2011, Trento, Italy)

Page 23: aircraft and tower eddy covariance flux measurements

(relative) wind measurement

differential & static pressures

Dynamic pressure

SSOS- Summer School on Optical Sampling  (7-13 July 2011, Trento, Italy)

Page 24: aircraft and tower eddy covariance flux measurements

SkyArrow ERA: wind measurement principle

SSOS- Summer School on Optical Sampling  (7-13 July 2011, Trento, Italy)

Page 25: aircraft and tower eddy covariance flux measurements

Aircraft motion measurement

Sistema alternativo (NOAA, IATA): Attitude GPS + accelerometri

Attitude 3D GPS a 4 antenne (10 Hz)

accelerometri (50 Hz)SSOS- Summer School on Optical Sampling  (7-13 July 2011, Trento, Italy)

Page 26: aircraft and tower eddy covariance flux measurements

Pressures50 HzGPS

Ground GPS

PositionVelocity

10Hz

Actual 3D wind retrieval

Accelerometers 50Hz

Attitude GPSAttitude10Hz

PositionVelocityAttitude50Hz

Actual 3D wind50Hz

SSOS- Summer School on Optical Sampling  (7-13 July 2011, Trento, Italy)

Page 27: aircraft and tower eddy covariance flux measurements

System calibration

IRGA Gas Analyzer

Pressure Ports

SSOS- Summer School on Optical Sampling  (7-13 July 2011, Trento, Italy)

Page 28: aircraft and tower eddy covariance flux measurements

The productsThe products

3D wind + scalar (T, H2O, CO2) fast measurements (50 Hz)

(eddy covariance tecnique)

Surface fluxes along flight track(u*, H, LE, fCO2)

SSOS- Summer School on Optical Sampling  (7-13 July 2011, Trento, Italy)

Flux transect over NL (Gioli et al 2006)

Page 29: aircraft and tower eddy covariance flux measurements

Tower data – 30 min continuous data

Aircraft data – ‘Spatial’ Fluxes

Data characteristics

SSOS- Summer School on Optical Sampling  (7-13 July 2011, Trento, Italy)

Page 30: aircraft and tower eddy covariance flux measurements

Footprint concept & aircraft fluxes

SSOS- Summer School on Optical Sampling  (7-13 July 2011, Trento, Italy) SSOS- Summer School on Optical Sampling

 (7-13 July 2011, Trento, Italy)

Page 31: aircraft and tower eddy covariance flux measurements

Validation of aircraft flux measurements

SSOS- Summer School on Optical Sampling  (7-13 July 2011, Trento, Italy)

Page 32: aircraft and tower eddy covariance flux measurements

Vellinga et al 2010

Regional C-budgets

SSOS- Summer School on Optical Sampling  (7-13 July 2011, Trento, Italy)

Page 33: aircraft and tower eddy covariance flux measurements

Validation of RS-based surface schemes at regional scale

SSOS- Summer School on Optical Sampling  (7-13 July 2011, Trento, Italy)

Page 34: aircraft and tower eddy covariance flux measurements

Some conclusions part 1 & 2

• eddy covariance widely used to measure surface fluxes across biomes, at high temporal resolution

• limitations arise from potential flux loss, & not perfect conditions (orography, inhomogeneities, low turbulence at night...)

• EC measures NEE, while GPP needs to be retrieved trough Reco estimation at nigh time (difficult...)

• EC can be succefully applied from aircraft platform and regional scale fluxes measured

SSOS- Summer School on Optical Sampling  (7-13 July 2011, Trento, Italy)

Page 35: aircraft and tower eddy covariance flux measurements

3. FLUX 3. FLUX MANIPULATION MANIPULATION

EXPERIMENTEXPERIMENT

SSOS- Summer School on Optical Sampling  (7-13 July 2011, Trento, Italy)

Page 36: aircraft and tower eddy covariance flux measurements

Surface energy balance

Rn = SW↓ +LW ↓ - SW↑ -LW↑ (net radiation)

Rn = H + LE + G

H: sensible heat flux (EC measured)

LE: latent heat flux = evapotranspiration (EC measured)

G = soil heat flux (measured)

SSOS- Summer School on Optical Sampling  (7-13 July 2011, Trento, Italy)

Page 37: aircraft and tower eddy covariance flux measurements

Study area

Page 38: aircraft and tower eddy covariance flux measurements

FLUX MANIPULATION EXPERIMENTFLUX MANIPULATION EXPERIMENT

Rn

HLE

G

H?

LE ?

G

CONTROL TREATMENT

(antitranspirant)Measurements:

H, LE, G (eddy towers)

Ts (IR camera on aircraft)

VIS-NIR (ground + aircraft) SSOS- Summer School on Optical Sampling  (7-13 July 2011, Trento, Italy)

Page 39: aircraft and tower eddy covariance flux measurements

can we observe a decrease in LE ?

can we observe an increase in H ?

can we observe an increase in Ts ?

how is VIS-NIR reflectance affected ?

how is photosynthesis affected ?

Can we observe change in energy partioning by eddy covariance & remote sensing ?

SSOS- Summer School on Optical Sampling  (7-13 July 2011, Trento, Italy)

Page 40: aircraft and tower eddy covariance flux measurements

4TE

T

bmax

Measuring Ts with thermal remote sensing

• IR camera detects 7.5 – 12 micron

• emissivity needed to estimate Ts

Wien's displacement law

Stefan–Boltzmann law

SSOS- Summer School on Optical Sampling  (7-13 July 2011, Trento, Italy)

Page 41: aircraft and tower eddy covariance flux measurements

Eddy covariance can be used to measure both resistances:

H, LE Penman Monteith equation rc (stomatal resistance)

u, u* aerodynamic resistance

H = Cp (Ts – Ta) / Rtot

Rtot = Rsto + Rnsto (total resistance)Rsto = resistance for water to be transpired trough stomataRnsto = other resistance (aerodynamic)

/)/)/)()((( aaaspnc rEreecGRr

Using Ts to assess surface energy balance

Page 42: aircraft and tower eddy covariance flux measurements

Feedbacks in the coupled land-atmosphere system

van Heerwaarden et al, 2009

positive feedback

negative feedback

at plot scale:

atmosphere surface (plot)

at larger scale:

atmosphere surface (region)

why is surface energy balance important ?


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