HAL Id: hal-02820244
https://hal.inrae.fr/hal-02820244
Submitted on 6 Jun 2020
HAL is a multi-disciplinary open access archive for the deposit and dissemination of sci- entific research documents, whether they are pub- lished or not. The documents may come from teaching and research institutions in France or abroad, or from public or private research centers.
L’archive ouverte pluridisciplinaire HAL, est destinée au dépôt et à la diffusion de documents scientifiques de niveau recherche, publiés ou non, émanant des établissements d’enseignement et de recherche français ou étrangers, des laboratoires publics ou privés.
The effect of LAI on the representativeness of eddy covariance estimates of ecosystem respiration during
turbulent conditions at night across a range of sites
May Myklebust, G. Wohlfahrt, Laurent Misson, Roland Huc, N. Delpierre, L.E. Hipps, R.J. Ryel, M.A. Arain, Michael Bahn, C. Bernhofer, et al.
To cite this version:
May Myklebust, G. Wohlfahrt, Laurent Misson, Roland Huc, N. Delpierre, et al.. The effect of
LAI on the representativeness of eddy covariance estimates of ecosystem respiration during turbulent
conditions at night across a range of sites. European Geosciences Union General Assembly 2009, Apr
2009, Vienne, Austria. 1 p., 2009. �hal-02820244�
M.C. Myklebust a *, G. Wohlfahrt b , L. Misson c , R. Huc a , N. Delpierre d , L.E. Hipps e , R.J. Ryel f , M.A. Arain g , M. Bahn b , C. Bernhofer h , B. Chojnicki i , P. Curtis j , S. Frokling k , P. Lafleur l , B. Longdoz m , E. van Gorsel n M. Aurela o , P., M. Cavaleri p , A.R. Desai q , A. Ito r , H.W. Loescher s , S. Oberbauer t , J. Pumpanen u , M.G. Ryan v , N. Saigusa w , T. Vesala x , C. Yi y
Objectives Introduction
The effect of LAI on the representativeness of eddy covariance estimates of ecosystem respiration during turbulent conditions at night across a range of sites
Calm conditions at night cause eddy covariance (EC) systems to underestimate ecosystem respiration (R ECO ) due to poor mixing of the canopy air. However, turbulent conditions do not always result in reliable nighttime measurements either. Decoupling at night in turbulent conditions can be explained by the difference between the adjustment lengths for momentum and heat transfer in the canopy (Belcher et al., 2008) or by drag imposed on moving air by canopy elements (Yi, 2008). Both explanations lead to storage, the development of horizontal and vertical gradients, and advective processes in the air within and below the canopy. Overall, these processes can cause EC to underestimate R ECO and suggests that the potential for underestimating may depend on leaf area index (LAI). This study investigated the effect of LAI on the representativeness of EC measurements of R ECO at night in turbulent conditions (R EC ) in a wide range of vegetation types, climates, and topographies.
EC-independent estimates of R ECO (R ALT ) often have very large uncertainties and therefore, are difficult to use for the evaluation of R EC . But R ALT
estimates can be assumed to have random errors that cancel when pooled. In contrast, errors in R EC due to an effect of LAI are assumed to be systematic.
We used R ALT to test R EC representativeness (R ACC ) by RE C – R ALT = R ACC over a range of LAI from sites around the world.
Assess whether LAI effects R ACC by:
1.. Test for a common trend in R ACC over LAI at sites with seasonal or annual changes in LAI.
2. Test for a trend in R ACC with LAI across multiple sites.
Methods
R EC : Turbulence fluxes of CO 2 were determined from high frequency measurements of CO 2 density and wind speed in 3 dimensions. Only data from nights when turbulence intensity (u*) was above a site-specific threshold were used.
c
y = 0.43x - 0.28 R2 = 0.17
-8 -6 -4 -2 0 2 4 6 8 10
0 2 4 6 8 10
RACC (CO2 μmol m-2 s-1)
Results
While R EC underestimates at some sites in turbulent conditions at night, we found no evidence for a general underestimation in these conditions when results are pooled across sites. This implies that EC generates realistic to slightly underestimated approximations of R ECO when multiple ecosystems are considered.
The nighttime problem with EC estimates is seen at certain sites. We showed that these sites are not confined to certain vegetation structure or topography classes but may predominate in situations where vapor pressure deficit and transpiration rate are both high. This suggests that water vapor may play a role in canopy air movement at night.
R ALT : Several methods were used to estimate R ALT . The only criteria was that they needed to be completely independent of R EC . Scaled up measurements of leaf and soil respiration, modeled R ECO and a combination of the two methods were used (table 1).
1. Mainly insignificant relationships between R ACC and LAI across 6 of 8 sites of various vegetation structure and topography suggest that LAI does not directly effect R EC . Two sites, US-MAL (a) and US_BLO (h) indicate LAI correlation with R EC underestimation (p≤0.1). These sites differ in vegetation structure and topography but share a similar climate (semi-arid) and both species transpire at night.
Conclusion
n
Finnish Meteorological Institute, Climate and Global Change Research, P.O. Box 503, Helsinki, FIN 00101 Finland
oCSIRO Marine and Atmospheric Research, Pye Laboratory, GPO Box 3023, Canberra ACT 2601, Austrailia
pBotany Department, University of Hawaii, 3190 Mali Way, Honolulu, HI 96822 USA
q
Atmospheric and Oceanic Sciences Department, University of Wisconsin, AOSS 1549, 1225 W Dayton St., Madison, WI 53706 USA
rFrontier Research Center for Global Change, JAMSTEC, Yokohama, Japan, National Institute for Environmental Studies, Tsukuba, Japan
sThe National Ecological Observatory Network (NEON), Science Office, Boulder CO 80303, and Institute for Arctic and Alpine Research,
University of Colorado, Boulder, CO, USA
tDepartment of Biological Sciences, Florida International University, Miami, FL 33199 USA
uDepartment of Forest Ecology, P.O. Box 27, University of Helsinki, FIN 00014, Finland
vUSDA Forest Service, Rocky Mountain Research Station, Fort Collins, CO 80526-2098 USA
wNational Institute for Environmental Studies, 16-2 Onogawa, Tsukuba 305-8506, Japan
xDepartment of Physics, P.O. Box 64, University of Helsinki, FIN 00014, Finland
y
School of Earth and Environmental Sciences, Queens College, City University of New York, NY 11367, USA
aInstitut National de la Recherche Agronomique, Ecologie des Forêts Méditerranéennes, UR 629, 84914 Avignon, France
b
Institute of Ecology, University of Innsbruck, Sternwartestr. 15, 6020 Innsbruck, Austria
cCNRS-CEFE, 1919 Route de Mende, 34293 Montpellier Cedex 5, France
d
Université Paris-Sud, Département Ecophysiologie Végétale, Ecologie Systématique, Evolution (UMR 8079), 91405 Orsay, France
eDepartment of Plants, Soils, and Climate, Utah State University, Logan, UT, USA 84322-4820
f
Department of Wildland Resources, Utah State University, Logan, UT, 84322-5230 USA
efEcology Center, Utah State University, Logan UT, 84322-5205, USA
g
McMaster University, School of Geography and Earth Sciences, 1280 Main Street, West Hamilton, ON L8S 4K1 Canada
hInstitute of Hydrology and Meteorology, Technische Universität Dresden, D-01737 Tharandt, Germany
iPoznan University of Life Sciences, 60-637 Poznan, Poland
j
Department of Evolution, Ecology, and Organismal Biology, Ohio State University, Columbus, OH 43210-1293 USA
kInstitute for the study of Earth, Oceans, and Space, University of New Hampshire, Durham, NH USA
lDepartment of Geography, Trent University, Peterborough, Ontario, Canada K9J 7B8
lUMR INRA-UHP 1137 Ecologie et Ecophysiologie Forestières, 54280 Champenoux, France
Grasslands
Wetlands
Broadleaf/mixed Forests
Needleleaf Forests
a
*y = 14.52x - 5.93 R2 = 0.61
-8 -6 -4 -2 0 2 4 6 8 10
0 2 4 6 8 10
RACC (CO2 μmol m-2 s-1)
e
y = -0.10x - 0.21 R2 = 0.15
-8 -6 -4 -2 0 2 4 6 8 10
0 2 4 6 8 10
RACC (CO2 μmol m-2 s-1)
g
y = -0.20x + 1.59 R2 = 0.18
-8 -6 -4 -2 0 2 4 6 8 10
0 2 4 6 8 10
PLAI RACC (CO2 μmol m-2 s-1)
b
y = 0.25x - 1.33 R2 = 0.13
-8 -6 -4 -2 0 2 4 6 8 10
0 2 4 6 8 10
d
y = 2.41x - 1.86 R2 = 0.49
-8 -6 -4 -2 0 2 4 6 8 10
0 2 4 6 8 10
f
y = 0.92x - 1.47 R2 = 0.60
-8 -6 -4 -2 0 2 4 6 8 10
0 2 4 6 8 10
h
y = 1.27x - 3.80 R2 = 0.73
-8 -6 -4 -2 0 2 4 6 8 10
0 2 4 6 8 10
PLAI RACC (μmol m2 m-2)