HAL Id: hal-02826914
https://hal.inrae.fr/hal-02826914
Submitted on 7 Jun 2020
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introduced by the measurements systems
Bernard Longdoz
To cite this version:
Bernard Longdoz. EC for measuring soil CO2 efflux and disturbances introduced by the measurements systems. ESF-summer school on ”Integrated methodology on soil carbon flux measurements”, Sep 2004, Monte Bondone, Italy. 34 p. �hal-02826914�
Bernard LONGDOZ
UMR Écologie et Écophysiologie Forestière
Institut National de la Recherche Agronomique (INRA) Centre de Nancy
FRANCE
E-mail : longdoz@nancy.inra.fr
Eddy Covariance, Forest soil CO2 efflux, fluxes canopy model
EC for measuring soil CO2 efflux &
Disturbances introduced by the
CO2 budget for a control air volume: • Source(s)
• Sink(s)
• Accumulation
• Transport by wind (advection, turbulence) • Molecular diffusion
Eddy Covariance
• Storage
• vertical & horizontal turbulence
• vertical & horizontal advection
• Molecular diffusion
• Storage
• vert. & hor. turbulence
• vert. & hor. advection
• molecular diffusion • horizontal homogeneity • No mean vert. w at soil surface • few cm height: turb. >>> diffusion
height cm tens few at flux turbulent vertical Rs =
w : vertical wind component
C : [CO2]
‘ : variance, high frequency oscillations around the time average (turbulence)
_
(
w ⋅'C')
at few tenscm height=
(vert. turbulence + molecular diffusion)soil surf
= (vert. turbulence + vert. advection)few cm + storage
= Rs Usually at few tens cm height :
Main material composing EC system : • High frequency 3D sonic anemometer • High frequency gas analyser
Measurements of
• 3 wind speed components
• [CO2]
at high frequency (above 10 Hz):
(
w'C')
sonic anemometer
Closed path IRGA
Open path IRGA
Limitations
Usually: vertical turbulent flux >>>
vertical advection + storage
Except during low turbulence period (low u*)
(quiet nights, below closed canopy) 0 0.5 1 1.5 0 0.2 0.4 0.6 0.8 1 1.2 FRICTION VELOCITY u* [m/s] N O R M A L IS E D F L U X [ -]
Disturbances introduced by the
measurement system
Introduction of measurement system
disturbances of natural process
Soil CO2 efflux measurement system
disturbances of CO2 flux going out of soil surface
How production and diffusion can be disturbed ?
Which variables controls soil CO2 efflux ?
How experimental system change variables values ? How reduce and correct these changes ?
(reduce the impact, correction)
Variables controlling the soil CO
2efflux
∆C<<< Rs Rs = Fc
Fc : wind transport (turbulence) +
molecular diffusion
Momentum conservation equation
vz depends on δP/δz and vh (2)
(
)
mol c z V z C D C v Fc Rs δ δ − = =vz : vertical wind speed
C : [CO2]
δC/δz : vertical [CO2] gradient
Dc : CO2 molecular diffusivity
Vmol : molar volume
(Lund et al., 1999)
(1) + (2) Rs function of δP/δz, δC/δz and vh
Conclusion :
Ideal measurement system should reproduce the natural
distributions of the δP/δz, δC/δz and vh
Perturbations of the δP/δz, δC/δz and vh by chambers
(open, closed dynamic/static), EC and gradient method
δP/δz : pumping effect, wind transport
δC/δz : diffusion
δ
P/δz
No perturbations by EC, gradient method and closed static chambers
Possible perturbations with closed dynamic and open chambers (pump)
Closed dynamic chambers
• Pump creates overpres. and depres.
• Air circulates along pressure gradient • Pressure in chamber fct(chb. position
PDC = Pch - Patm 0 pumping effect PDC = ± few Pa ??? Important ??? 0.0 0.5 1.0 1.5 2.0 2.5 3.0 3.5 4.0 -3 -2 -1 0 1 2 3 PDC (Pa) N or m al is ed s oi l C O2 e ff lu x exp {-0.41 PDC} Data from the Vielsalm forest site
(Belgium) PDC = -0.5 Pa Rs +20% PDC = +0.2 Pa Rs -9% Yes Sensitivity depend on
Soil porosity Soil productivitySensitivity increase with Sensitivity increase with
Fang & Moncrieff
(1998)
Rs +510% Rs -44%
Grassland & crops : potential disturbance Solution P < Patm P > Patm Leak <<< soil CO2 efflux
Another leak important PDC
Check regularly PDC
High frequency oscillations of Patm not reproduced
Study of the impact in progress (Takle & al 2004 AFM) Another source PDC :
• fan for [CO2] homogeneity
PDC > 1 Pa in the centre PDC < -0.5 Pa around solution : metal grid at the chamber bottom • heating of transparent chamber (up to 15°C)
air dilatation positive PDC
PDC in open chamber • 1 pump
PDC exist but
• 2 pumps
Solution : 2 mass flow controllers
δ
C/δz
No perturbations by EC
Possible perturbations with gradient method, closed static chambers, closed dynamic and open chambers
Gradient method
Bad insertion of tube in soil
Closed dynamic chamber 0 0.2 0.4 0.6 0.8 1 1.2 0 50 100 150 200 250 300 350 Time (s) C O 2 e ff lu x ( g m -2 h -1 ) 360 365 370 375 380 385 390 C O 2 (µ m o l m o l -1 )
[CO2]ch > [CO2]atm
or
[CO2]ch from below to
above [CO2]atm (scrub)
Efflux increase if [CO2]ch < [CO2]atm
Efflux decrease if [CO2]ch > [CO2]atm
δ
C/δz
disturbance
Recommendation :
Determine the [CO2] thresholds to neglect slope variations
(work in this interval or correction)
Closed static chamber
If chemical traps: [CO2]ch
↗
↗
↗
↗
until Rs = trap absorptionRs underestimated If sample same that dynamic without scrub
0 0.2 0.4 0.6 0.8 1 1.2 0 50 100 150 200 250 300 350 Time (s) C O2 e ff lu x ( g m -2 h -1 ) 360 365 370 375 380 385 390 C O 2 (µ m o l m o l -1 ) Open chamber
Inlet: [CO2]atm
In chamber [CO2]
↗
↗
↗
↗
[CO2]ch > [CO2]atm
Same
recommendation
For all chambers
Insertion of the collar roots cut Csoil (
δ
C/δz
) perturbedv
hNo perturbations by EC and gradient method
Unable to reproduce
v
h in closed static/dynamic and openchambers
closed static chamber
v
h = 0closed dynamic and open chambers
Difficult to separate from pressure disturbance !!! Longdoz et al., 2000 :
PDC and [CO2]ch corrections
Experimental Design
Experimental design adapted to :
• Ecosystem (grassland , forest, crops) • Spatial scale
• Temporal scale Grassland
EC & all chambers : no separation grass
↮
soilForest
Chambers, gradient method, EC (with selection on u*) Crops
EC : no separation vegetation
↮
soilSpatial scale 0 0.5 1 1.5 2 2.5 3 3.5 3 5 7 9 LAI R 1 0 Interplot variability
0 10 20 30 40 50 60 0.5-1.0 1.0-1.5 1.5-2.0 2.0-2.5 2.5-3.0 3.0-3.5 3.5-4.0 4.0-4.5 4.5-5.0 5.0-5.5 5.5-6.0 Fs10 (µmol m-2 s-1) F re qu en cy ( % ) Beech Douglas fir Intraplot variability
EC : few m2
gradient : few dm2
open chamber : few dm2
manual closed dynamic chamber : plots moved by experimenter
0 1 2 3 4 5 6 15/8 14/9 14/10 14/11 14/12 14/1 13/2 15/3 15/4 15/5 15/6 15/7 S pa ti al m ea n so il C O2 e ff lu x ( µm ol m -2 s -1 ) simulated measured Temporal scale
Inter-annual (long term) Seasonal
Année 2002 50 100 150 200 250 300 350 0 1 2 3 4 0 5 10 15 20 Flux Température du sol Jours juliens F lu x d e C O2 ( µ m o l. m -2 .s -1 ) T e m p é ra tu re m o y e n n e d u s o l ( °C ) Day to day
-0.5000 0.0000 0.5000 1.0000 1.5000 2.0000 2.5000 3.0000 3.5000 4.0000
3-juil-2001 4-juil -2001 5-juil -2001 6-juil -2001 7-juil-2001 8-juil-2001 9-juil-2001 10-juil-2001 11-juil-2001 12-juil-2001 13-juil-2001
Jours F lu x d e C O 2 ( µ m o l. m -2 .s -1 ) 0.00 0.05 0.10 0.15 0.20 0.25 0.30 0.35 0.40 0.45 0.50 H u m id it é d u s o l (m 3 .m -3 ) e t p lu ie ( l. m -2 ) Half-hour
EC : half-hour on long term
open chamber : half-hour on short term (days) gradient : half-hour on long term
manual closed dynamic chamber :
day to day seasonal variation automatic closed dynamic chamber :
Topic for discussion (proposal)
automatic closed dynamic chamber + gradient
separation of CO2 production and diffusion