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Jökull - 01.12.1994, Qupperneq 21

Jökull - 01.12.1994, Qupperneq 21
tonic units that comprise the Hengill triple junction thus affect the seismicity, volcanism and spreading and consequently the deformation, but are not yet fully understood. GPSSURVEYING The GPS system, operation and its use as a geode- tic tool is described fully by Wells (19S7), King et al. (1985) and Leick (1991). For maximum precision surveying, both P-code and phase measurements are recorded on both frequencies. Combination of the two frequencies enables correction for the variable effect of ionospheric refraction, a major problem in Iceland because of its high latitude. The effect of the tropo- sphere may be corrected for using a standard tropo- sphere model at the data processing stage. Field measurements are conducted by erecting a GPS receiver antenna over a ground control point and recording data. Receivers are deployed simultaneously at more than one point and data recorded from com- mon satellites. The data are subsequently processed in- terferometrically and, knowing the absolute position of one point, the three-dimensional vector connecting it to other points may be calculated. From these the abso- lute coordinates of the other points may be derived. EARTH TIDES AND OCEAN LOADING Ocean tides cause changes in the gravitational po- tential on land by loading and deformation of the sea floor by the redistribution of water. In coastal areas the deformation due to ocean loading will greatly ex- ceed the effect of the Earth tides (Kuo et al., 1970). Deformation as a result of ocean tidal loading causes periodic variations in the relative positions of points on the Earth's surface by a few centimetres vertically and a few millimetres horizontally. Line lengths may therefore vary on a diumal basis and this represents an additional error source in GPS surveying hitherto generally ignored. To capture the ocean loading effect one must compare coordinates at particular instances throughout the cycle since the effect would tend to av- erage out if a session which covered most of the tidal cycle were used. The magnitude of the loading is difficult to esti- mate as tides in the open ocean are poorly known and often can only be inferred from data at coastal sta- tions. Wu-Ling and Morgan (unpublished computer program) compute vertical and horizontal movements over the surface of the Earth resulting from ocean loading by convolving Schwiderski's tidal model with Farrel's load Green's function (Schwiderski, 1980; Farrel, 1972). Schwiderski's model divides the open oceans into 1 x 1 degree squares. For each square there are 11 different partial wave functions, the largest of which is the Principal Lunar Semi-diumal Tide (M2). Schwiderski's model yields 66 deforma- tion constants for each node on the grid. These are six deformation constants for each of the 11 partial wave functions, a sine and cosine term representing defor- mation in the north, east, and up components. By summing these, theoretical vertical and horizontal de- formations at a point may be calculated. Figure 2 shows the maximum vertical displace- ments over Iceland with respect to reference stations at Reykjavík, Akureyri, Búrfell and Borgarfjörður. The variation in the height difference between two points increases almost linearly with distance. The variation could be as much as 140 mm if the baseline spanned the island, e.g. Reykjavík to Bakkagerði (Figure 2a), and 130 mm between points in the interi- or and on the coast, (Figure 2c). DESIGN AND MEASUREMENT OF THE HENGILL GPS NETWORK In August 1991 a 23-point GPS network was es- tablished and measured in an area 750 km2 in and around the Hengill triple junction. The point positions were selected to achieve fairly uniform coverage of the Hengill triple junction including all three volcanic systems and the transform branch in Ölfus. Twenty of the points were newly installed by cementing brass pegs into stable bedrock. Five points were preexisting GPS points and two were old triangulation monu- ments (Fig. 3, Table 1). The network was measured using three C/A code Ashtech dual frequency re- ceivers. The receivers recorded the C/A code, full wavelength phase measurements on L1 and half- JÖKULL, No. 44 19
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