Air samples were taken concurrently for four sampling events in the winter
of 1998 at three contrasting sites: an urban center and two rural sites. Th
e rural sites were characterized by the extensive usage of coal and wood fo
r space heating. Samples were analyzed for PCDD/Fs, PCBs, and PAHs. Recentl
y measured octanol-air partition coefficients (K-oa) for PCDD/Fs enabled a
comparison of the K-oa-based versus the subcooled liquid vapor pressure (p(
L))-based partition model for all three compound classes. Both K-oa and p(L
) were found to be excellent descriptors of the gas-particle partitioning o
f PCDD/Fs, PCBs, and PAHs. However, regressions for log K-p-log p(L) gave h
igher regression coefficients than for log K-p-log K-oa. Both models showed
roughly similar relative states of equilibrium for PCDD/Fs, PCBs, and PAHs
. PCBs were closest to equilibrium at the urban site. It is argued that new
ly released particles at the rural sites caused nonequilibrium partitioning
at those sites for PCBs. PAHs were released at all sites and were, in line
with expectations, approaching equilibrium. The K-oa-based and the p(L)-ba
sed model gave contradictory results for PCDD/Fs: according to the p(L)-mod
el, PCDD/Fs were in equilibrium for event 1 but not for the other events, w
hereas the K-oa-model showed the PCDD/Fs not being in equilibrium for event
1. A simple K-oa-model, combining advective transport and locally released
PCDD/Fs and PAHs, can explain the observed nonequilibrium partitioning for
the first sampling event.