A 25-year dataset of potential vorticity on the 315-K isentropic surfa
ce is built from the National Meteorological Center (NMC) final analys
is archive. potential vorticity is calculated from the nonlinear gradi
ent wind balance using temperature and geopotential fields, since the
wind field is not available in the early part of the archive. The vali
dity of this calculation is assessed by comparing the results with pot
ential vorticity obtained directly from European Centre for Medium-Ran
ge Weather Forecasts (ECMWF) analyzed winds. The error due to the nonl
inear balance approximation turns out to be smaller than the differenc
e between ECMWF and NMC analysis. The possibility of studying diabatic
forcing as a residual of the equation of potential vorticity conserva
tion is examined. The average potential vorticity forcing found in thi
s way is consistent with the authors knowledge of the mean diabatic he
ating. The amplitude of the residual decreases through the analysis pe
riod, reflecting the improvement in the observational network and in t
he analysis schemes. Next the authors demonstrate that this dataset ca
n be used for studies of transient-mean flow interactions. The authors
present diagnostics of the transient feedback by separating the contr
ibution of vortical and thermal terms on the isentropic surface. Also,
the contribution of high-frequency (periods less than 10 days) and lo
w-frequency (periods greater than 10 days) transients is examined. On
the 315-K surface, transients act mostly in reducing the potential vor
ticity gradient through thermal terms and accelerate the zonal flow th
rough vortical forcing. Finally, these diagnostics are also applied to
a long ensemble of blocking events, and the authors study the anomaly
of transient feedback during these events. It is found that transient
s have primarily an advective effect, forcing the dipole structure to
retrograde westward. Thermal and vortical terms have a very distinct a
ction on the blocking anomaly. Vortical forcing is constructive and ad
vective, whereas thermal forcing is dissipative and makes the dipole r
otate clockwise.