J. Vogelzang et al., MAPPING SUBMARINE SAND WAVES WITH MULTIBAND IMAGING RADAR .2. EXPERIMENTAL RESULTS AND MODEL COMPARISON, J GEO RES-O, 102(C1), 1997, pp. 1183-1192
On August 16, 1989, and on July 12, 1991, experiments were performed t
o study the mapping of submarine sand waves with the airborne imaging
radar, a polarimetric (and, in 1991, interferometric) airborne P, L, a
nd C band synthetic aperture radar system. The experiments took place
in an area 30 km off the coast of the Netherlands, where the bottom to
pography is dominated by sand waves with a height between 2 and 6 m an
d a crest-to-crest distance of about 400 m at an average depth of 22 m
. Ground measurements were recorded on a nearby platform and on a ship
in the test area, which also acted as a position fix. On August 16, 1
989, the wind was 5 mis directed toward the northeast, while the surfa
ce current velocity was around 0.5 mis directed toward the southwest.
One overflight was made, with the flight direction parallel to the san
d wave crests and the radar looking upwind. At P band. the sand waves
are clearly visible as dark bands, as predicted by theory, while at L
band the sand waves show up as sawtooth-shaped modulations. On July 12
, 1991, wind and surface current had the same (opposite) directions as
in 1989, though the wind was much higher (10 mis). Three flights were
made, with the radar pointing upwind, cross wind, and downwind. The u
pwind and downwind images are very similar. Despite the high wind spee
d, the sand waves are clearly visible as sawtooth-shaped modulations a
t P band and vaguely visible at L band. At C band, only wind streaks c
an be seen. All cross wind images show the sand waves as dark bands, n
ow with the highest modulations at C band. The wind streaks that domin
ated the upwind and downwind images at C band are much less pronounced
in the cross wind images. The images are compared with predictions fr
om a new model of the imaging mechanism which includes contribution to
the radar cross section of waves moving both from and to the radar. W
ave blocking or wave reflection is treated in an approximate manner. F
or the radar looking upwind or downwind, the predicted modulations at
P and L band agree well with the observations, while those at C band a
re too high. For the radar looking crosswind, the model severely under
estimates the modulations. It is questioned whether a local relaxation
source term can describe such a situation. The interferogram shows so
me structure caused by bottom-induced surface current variations.