Lf. Bosart et al., A STUDY OF CYCLONE MESOSCALE STRUCTURE WITH EMPHASIS ON A LARGE-AMPLITUDE INERTIA-GRAVITY WAVE, Monthly weather review, 126(6), 1998, pp. 1497-1527
analysis is presented of prominent mesoscale structure in a moderately
intense cyclone with emphasis on a long-lived, large-amplitude inerti
a-gravity wave (IGW) that moved through the northeastern United States
on 4 January 1994. Available National Weather Service WSR-88D Doppler
radar and wind profiler observations are employed to illustrate the r
ich, time-dependent, three-dimensional structure of the IGW. As the IG
W amplified [peak crest-to-trough pressure falls exceeded 13 hPa (30 m
in)(-1)], it also accelerated away from the cyclone, reaching a peak f
orward speed of 35-40 m s(-1) across eastern New England. The IGW was
one of three prominent mesoscale features associated with the cyclone,
the others being a weak offshore precursor warm-frontal wave and an o
nshore band of heavy snow (''snow bomb'') in which peak hourly snowfal
ls of 10-15 cm were observed. None of these three prominent mesoscale
features were well forecast by existing operational prediction models,
particularly with regard to precipitation amount, onset, and duration
. The observed precipitation discrepancies illustrate the subtle but i
mportant effects of subsynoptic-scale disturbances embedded within the
larger-scale cyclonic circulation. The precursor offshore warm-fronta
l wave was instrumental in reinforcing the wave duct preceding the IGW
. The snow bomb was an indication of vigorous ascent, large upper- (lo
wer-) level divergence (convergence), unbalanced flow, and associated
large parcel accelerations, environmental conditions known to be favor
able for IGW formation. Small-amplitude IGWs (<1 hPa) are first detect
ed over the southeastern United States from surface micro-barogram rec
ords and are confirmed independently by the presence of organized and
persistent mesoscale cloud bands oriented approximately along the wave
fronts. The area of IGW genesis is situated poleward of a weak surfac
e frontal boundary where there is a weak wave duct (stable layer) pres
ent in the lower troposphere. In the upper troposphere the region of I
GW genesis is situated on the forward side of a deep trough where ther
e is significant cyclonic vorticity advection by the thermal wind. Dia
gnostic evidence supports the importance of shearing instability and/o
r unbalanced flow in IGW genesis. The large-amplitude IGW originates o
n the downstream edge of the northeastward-advancing packet of small-a
mplitude IGWs. Wave amplification occurs near the upshear edge of a hi
gh, cold cloud shield that generally marks the warm conveyor belt. Alt
hough it is not possible to conclusively state whether the amplifying
IGW forms in situ or grows from a predecessor weaker (<1 hPa) disturba
nce, rapid amplification occurs 1) as the wave encounters an increasin
gly deeper and stronger wave duct, possibly permitting wave overreflec
tion, in the cold air damming region east of the Appalachians, and 2)
downshear of an area of significantly positive unbalanced divergence a
nd parcel divergence tendency. The authors raise the possibility that
IGW amplification can be associated with the penetration and perturbat
ion of the wave duct by vigorous subsynoptic-scale vertical motions wh
ose vigor is increased by wave-induced latent heat release.