VIDEO/LASER HELICOPTER SENSOR TO COLLECT PACK ICE PROPERTIES FOR VALIDATION OF RADARSAT SAR BACKSCATTER VALUES

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VIDEO/LASER HELICOPTER SENSOR TO COLLECT PACK ICE PROPERTIES FOR VALIDATION OF RADARSAT SAR BACKSCATTER VALUES S.J. Prinsenberg 1, I.K. Peterson 1 and L. Lalumiere 2 1 Bedford Institute of Oceanography, Dartmouth, Nova Scotia, Canada. 2 Sensors by Design Ltd., Newmarket, Ontario, Canada. ABSTRACT A helicopter-mounted Video-Laser-GPS system was used to collect video images and surface roughness data from the Gulf of St. Lawrence pack ice to validate the effect of the pack ice properties on the RADARSAT backscatter values in the RADARSAT ScanSAR Wide images. As ice floes become smaller than the pixel size (m) of the RADARSAT ScanSAR Wide image, the pixel backscatter properties not only depend on ice properties but also on the fraction of open water within the pixel. To study the dependence of the SAR backscatter on ice concentration as well as on the floe size distribution and surface roughness, the video/laser data was collected from pack ice areas with different backscatter values. GPS-ARGOS ice beacons deployed on ice floes provided hourly ice velocities to co-register the imagery with the helicopter-borne sensor data. Two SAR image examples are shown; one from Northumberland Strait of February 20, 1998 when the backscatter properties of the pack ice were deformed by the Bridge piers. The second example is from the marginal ice zone of March 13, 1998 where dynamic processes affect the sub-pixel roughness and ice concentration of the pack ice. 1. INTRODUCTION Winter navigation in Canadian waters relies heavily on ice information that can be extracted from remotely sensed data especially RADARSAT SAR imagery, as ice reconnaissance flights by fixed-wing or helicopter are costly, weather dependent and spatial restrictive. To improve the interpretation of RADARSAT SAR imagery, reconnaissance flights are necessary to collect ground-truth ice property data. In Canada, helicopter-borne sensors have been developed to optimize both the quality and quantity that can be collected during helicopter reconnaissance flights. One such sensor is an electromagnetic (EM) induction system (Rossiter and Holladay, 1994) which collects snow-plus-ice thickness and surface roughness data. Results of its uses in Radarsat validation are reported in Peterson et al. (1999, this issue). The other sensor is a Video-Laser-GPS system that is capable of collecting floe size distribution, ice concentration and surface roughness data. This note will describe the data collected by this second sensor during the winter of 1998 in the southern Gulf of St. Lawrence.

49 48 47 46-66 -64-62 -60 Figure. 1. RADARSAT ScanSAR Wide sub-scene acquired in February 20, 1998 (22:08Z) showing Northumberland Strait. The inset shows the area of the southern Gulf of St. Lawrence covered by the image. CSA/ASC, 1998. 2. FIELD SURVEY In February-March 1998, a field program was conducted out of Charlottetown, Prince Edward Island (P.E.I.) to collect ice property data to validate signatures seen in the RADARSAT SAR imagery from the southern Gulf of St. Lawrence. Some of the survey work was done south of P.E.I. in Northumberland Strait where the 13km long Confederation Bridge has recently been completed (narrow section of the strait, linking the two white dots in Figure 1). The Video system frame-grabs digital video images and logs laser altimeter profiles along with GPS

position data. The system uses the expected flying height, flying speed, field of view and frame size to establish the frame capture rate which ranges from 0.5sec when flying at m to 3.0sec at 300m (0ft). Since the video frame has 240x320 pixels and the video frame view width is approximately equal to the flying height, the video pixel size is about 15cm when flying at m and 1m when flying at 300m. GPS data are logged at 1/sec, radar altimeter at 10/sec and laser altimeter at 30/sec. ARGOS satellite-tracked GPS ice beacons were deployed on ice floes to monitor ice drift. Hourly GPS-derived position data from the beacons were telemetered via Service ARGOS and have an accuracy of about 40m. 3. RESULTS The February 20 image shows that west of the bridge there exists an ice area with a high backscatter value which changes abruptly to low values when pack ice with floe sizes of 2 to 5km is encountered. The bridge piers cuts the pack ice into small floes (10 - m), as the ice moves back and forth past the bridge in response to tidal currents and wind forcing (Peterson et al., 1998a). The ice area affected by the bridge piers was monitored by satellite-tracked ice beacons which indicated that the pack ice moved 40km to the west under strong easterly winds from February 18 to 20 (Figure 2). Two beacons were placed west of the bridge on large floes unaffected by the bridge piers, while the other two beacons were placed east of the bridge on small floes already affected by the bridge piers. The area between the two pair of beacons thus track the demarcation line between large and small floes, which at the time of the image was 40km east of the Bridge. Beacon 2754 Beacon 2755 30' 30' 24' 53/0 24' 18' 12' 53/0 49/19 18' 12' 6' 49/20 6' 46 o N 64 o W 64 o W 46 o N Beacon 2756 Beacon 2757 30' 30' 24' 24' 18' 53/1 18' 12' 49/20 /6 49/21 12' 6' 6' 46 o N 64 o W 64 o W 46 o N Figure 2. Beacon trajectories between day 49, Feb. 18 (19:00-21:00AST) and day 53, Feb. 22 (01:00AST). Tidal ice motion is seen in trajectories of beacons #2754 and #2755. Beacon #2757 sunk while passing the bridge area on day (06:00AST) The relative brightness (grey level) of the image changes from of the unaffected pack ice (area A on Figure1) to 69 for the affected area west of the bridge where small, rough floes

are present (area B) and back to 62 for the area C east of the bridge where the small floes possibly occur at a lower ice concentration. The different backscatter brightness in RADARSAT imagery near the bridge is related to sub-pixel scale properties seen in the video images acquired on February 24 (Figure 3) while flying at a height of m along the Strait from west to east. Before the affected area west of the Bridge was reached large floes encompassed the entire video image (#2285). The ice in the other three images of Figure 3 is of same general ice type but has been fractured by the piers of the bridge; brash ice has also been produced in the open water areas between the floes. #2285 (11:05) #2410 (11:11) #2556 (11:18) #2700 (11:25) Figure 3. Video images from February 24, 1998 between 11:05AST and 11:25AST. The horizontal scale of the images is approximately m; equal the video height. Video image #2410 is from west of the Bridge and #2700 from east of the Bridge. Image #2556 shows the image while passing over the bridge. When the small floes occur in high ice concentration (#2410), the brightness in the RADARSAT image increases relative to unaffected areas (#2285). As more open water appears between the small floes (#2700), the backscatter decreases as low backscatter from the water (light winds) nullified the increase in

backscatter due to rough floe topography. The laser was not yet installed at this time of the survey, and thus no laser roughness data is available. March 13 1998 300 49 48 47 46-66 -64-62 -60 400 0 600 700 800 300 400 0 600 700 800 Figure 4. RADARSAT ScanSAR Wide scene from March 13, 1998 (21:57Z) covering the area north and northwest of PEI. The inset shows the area of the Gulf of St. Lawrence covered by the image and the rectangular sub-scene section shown in Figure 5. CSA/ASC, 1998. In the marginal ice zone, the small scale variation in pack ice roughness and ice concentration are caused by dynamic processes as the pack ice growths or decays. The RADARSAT image of March 13, 1998 (Figure 4) shows the video flight path that extended from the first year ice north of PEI, into the ice edge NW of PEI where smooth, new ice areas (dark areas on image) were encountered. Between the first year ice and the new ice area, the flight path passed over brash ice and some deformed floes (bright on the image). A sub-scene (Figure 5) shows the section of the flight path that passed over the bright image areas. The flight path was moved ESE by 2.9km for the estimated ice drift over the 1.5hr time difference between the SAR and video images. The ice drift was based on data from a GPS ice beacon about 7km east of the flight track. The pack ice roughness data collected by the laser at m altitude and the SAR brightness from the image along the track are shown in Figure 6. There is good agreement between the degree of surface roughness and the SAR brightness.

Pixel Number 1 2 300 3 400 4 751 701 651 601 551 1 451 401 351 301 251 201 151 101 300 400 0 Pixel Number Figure 5. RADARSAT ScanSAR Wide sub-scene from March 13, 1998 (21:57Z) for a 25kmx20km area with video numbers along flight track. CSA/ASC, 1998. 51 1 1 Laser Roughness (m) 0.8 0.6 0.4 0.2 0 1 51 101 151 201 251 301 351 401 451 1 551 601 651 701 751 Video Frame Number 1 RADARSAT Profiles (Normalized Brightness) 0.8 0.6 0.4 0.2 0 1 51 101 151 201 251 301 351 401 451 1 551 601 651 701 751 Video Frame Number Figure 6. Laser roughness and RADARSAT brightness profiles along the track shown in Figure 5, flown on March 13, 1998 between 20:20Z and 20:29Z.

#108 #287 #435 #678 Figure 7. Video images from March 13, 1998 between 20:20Z and 20:29Z. The horizontal scale of the video is approximately m; equal the video height. The darker areas along the track at the start (video images 75-190) and at the end of the track (video images >700) are from the smoother ice areas along the track. In contrast, the high roughness areas are associated with the brighter areas of the SAR image. In Figure 7, four examples are shown of the different ice properties along the track. The smooth level ice shown in image #108 is from the dark area (Figure 5) at the start of the track where low roughness values were observed by the laser (Figure 6). Video #287 represents the grey area of the SAR image and shows a mixture of brash ice and small rough floes. The brightest areas along the track represent rough, rafted and ridged ice (image #435), consolidated into large floes (% ice concentration). Ridging is most pronounced near the edges of the floes. Image # 678 shows the rough-to-smooth ice transition area with the younger and smoother ice farther along the track to the northeast. Presently the video data is stored as a colour image consisting of three 8-bit colour planes. Investigation is underway to determine what information will be lost if either the colours are combined in one single grey scale or if just one of the colour plane is retained. Figure 8 shows the four available grey scale images of the image #287 shown in Figure 7. The combined grey

scale is the sum of 0.299(red plane), 0.587(green plane) and 0.114(blue plane). It follows the sensitivity of the eye, which is most sensitive to the green part of the colour spectrum. One concern is that when one develops an automatic image analysis routine to determine such things as ridge frequencies and ice concentrations of various ice types, will shadows be properly identified as ice rather than as thin ice or open water. Figure 8 shows that the Blue colour plane does distinguishes the thin ice types the best from either the open water area (black) or from shadow areas (light grey). However ridges become less distinguishable in the blue colour plane than in any other colour or combine grey scale planes. For this example, the red colour plane appears the best plane to provide ridge information. One colour grey plane may thus not provide all the required information. Combined Grey Scale Red Colour Plane 1 1 1 2 300 1 2 300 Green Colour Plane Blue Colour Plane 1 1 1 2 300 1 2 300 Figure 8. Video image #287 (Figure 7) plotted as a grey scale version using a combined grey scale and the red, green and blue 8-bit colour planes.

4. CONCLUSION Video and laser data collected by the GPS-Video-Laser system show that for the same ice type, the ice concentration and ice roughness affects the brightness of the SAR backscatter with brighter areas of the pack ice associated with rougher and higher ice concentration for each pixel of the RADARSAT image. Floes fractured by bridge piers that are smaller than the ScanSar Wide pixel scale do occur in high ice concentration in Northumberland Strait and causes high back scatter values. Within the pack ice convergence causes ridging and rafting which when consolidates into large floes will have high backscatter values due to the high surface roughness. New and young ice, which formed in nearby open water areas, had low backscatter values due to low surface roughness as the ice formed during calm winds (no pancake ice). The GPS-Video-Laser system provides valuable data to validate ice signatures in SAR RADARSAT imagery; the tasks in hand now is to develop analysis techniques to extract useful ice information from the data in near real-time that can be made available to the marine shipping industry. 5. ACKNOWLEDGEMENTS This work was funded in part by the Federal Panel on Energy Research and Development. We thank Andy Maillet of the Can. Coast Guard, our colleagues from the Bedford Institute, and other participants of the project from the Canadian Coast Guard, Transport Canada, Canadian Ice Service and Canada Centre for Remote Sensing. 6. REFERENCES Peterson, I.K., Prinsenberg, S.J. and Maillet, A. 1998. 1997 Pack ice properties in Northumberland Strait. ISOPE 98: Proceedings of the 8 th International Offshore and Polar Engineering Conference, Montreal, Canada, Vol. 2, pp. 513-518. Peterson, I.K., Prinsenberg, S.J. and Holladay, J.S. 1999. Using a helicopter-borne EM-induction system to validate RADARSAT sea ice signatures. Proceedings of 15 th International Conference on Port and Ocean Engineering under Arctic Conditions, POAC 99, Helsinki, Finland, this issue. Rossiter, J.R. and Holladay, J.S. 1994. Ice-thickness measurement. In: Remote Sensing of Sea Ice and Icebergs. John Wiley and Sons, New York, pp. 41-176.