Canopy stomatal conductance (gsV) is commonly estimated from eddy covariance (EC) measurements of latent heat flux (LE) by inverting the Penman-Monteith (PM) equation. That method implicitly represents the sensible heat flux (H) as the residual of all other terms in the site energy budget – even though H is measured at least as accurately as LE at every EC site while the rest of the energy budget almost never is. We argue that gsV should instead be calculated from EC measurements of both H and LE, using the flux-gradient formulation that defines conductance and underlies the PM equation. The flux-gradient formulation dispenses with unnecessary assumptions, is conceptually simpler, and provides more accurate values of gsV for all plausible scenarios in which the measured energy budget fails to close, as is common at EC sites. The PM equation, on the other hand, contributes biases and erroneous spatial and temporal patterns to gsV, skewing its relationships with drivers such as light and vapor pressure deficit. To minimize the impact of the energy budget closure problem on the PM equation, it was previously proposed that the eddy fluxes should be corrected to close the long-term energy budget while preserving the Bowen ratio (B = H/LE). We show that such a flux correction does not fully remedy the PM equation but should produce accurate values of gsV when combined with the flux-gradient formulation.
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Calculating canopy stomatal conductance from eddy covariance measurements, in light of the energy budget closure problem
Abstract. Canopy stomatal conductance is commonly estimated fromeddy covariance measurements of the latent heat flux (LE) by inverting thePenman–Monteith equation. That method ignores eddy covariance measurementsof the sensible heat flux (H) and instead calculates H implicitly as theresidual of all other terms in the site energy budget. Here we show thatcanopy stomatal conductance is more accurately calculated from eddy covariance (EC)measurements of both H and LE using the flux–gradient equations that defineconductance and underlie the Penman–Monteith equation, especially when thesite energy budget fails to close due to pervasive biases in the eddy fluxesand/or the available energy. The flux–gradient formulation dispenses withunnecessary assumptions, is conceptually simpler, and is as or more accuratein all plausible scenarios. The inverted Penman–Monteith equation, on theother hand, contributes substantial biases and erroneous spatial andtemporal patterns to canopy stomatal conductance, skewing its relationshipswith drivers such as light and vapor pressure deficit.
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- PAR ID:
- 10252771
- Date Published:
- Journal Name:
- Biogeosciences
- Volume:
- 18
- Issue:
- 1
- ISSN:
- 1726-4189
- Page Range / eLocation ID:
- 13 to 24
- Format(s):
- Medium: X
- Sponsoring Org:
- National Science Foundation
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