The net ecosystem exchange of CO2 between forests and the atmosphere, measu
red by eddy covariance, is the small difference between two large fluxes of
photosynthesis and respiration. Chamber measurements of soil surface CO2 e
fflux (F-s), wood respiration (F-w,) and foliage respiration (F-f) help ide
ntify the contributions of these individual components to net ecosystem exc
hange. Models developed from the chamber data also provide independent esti
mates of respiration casts. We measured CO2 efflux with chambers periodical
ly in 1996-97 in a ponderosa pine forest in Oregon, scaled these measuremen
ts to the ecosystem, and computed annual totals for respiration by componen
t. We also compared estimated half-hourly ecosystem respiration at night (F
-nc) with eddy covariance measurements. Mean foliage respiration normalized
to 10 degrees C was 0.20 mu mol m(-2) (hemi-leaf surface area) s(-1), and
reached a maximum of 0.24 mu mol m(-2) HSA s(-1) between days 162 and 208.
Mean wood respiration normalized to 10 degrees C was 5.9 mu mol m(-3) sapwo
od s(-1), with slightly higher rates in mid-summer, when growth occurs. The
re was no significant difference (P > 0.10) between wood respiration of you
ng (45 years) and old trees (250 years). Soil surface respiration normalize
d to 10 degrees C ranged from 0.7 to 3.0 mu mol m(-2) (ground) s(-1) from d
ays 23 to 329, with the lowest rates in winter and highest rates in late sp
ring. Annual CO2 flux from soil surface, foliage and wood was 683, 157, and
54 g C m(-2) y(-1), with soil fluxes responsible for 76% of ecosystem resp
iration. The ratio of net primary production to gross primary production wa
s 0.45, consistent with values for conifer sites in Oregon and Australia, b
ut higher than values reported for boreal coniferous forests. Below-ground
carbon allocation (root turnover and respiration, estimated as F-s, - litte
rfall carbon) consumed 61% of GPP; high ratios such as this are typical of
sites with more water and nutrient constraints. The chamber estimates were
moderately correlated with change in CO2 storage in the canopy (F-stor) on
calm nights (friction velocity u* < 0.25 m s(-1); R-2 = 0.60); F-stor was n
ot significantly different from summed chamber estimates. On windy nights (
u* > 0.25 m s(-1)), the sum of turbulent flux measured above the canopy by
eddy covariance and Fstor Was only weakly correlated with summed chamber es
timates (R-2 = 0.14); the eddy covariance estimates were lower than chamber
estimates by 50%.