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Fig.3 Comparison of observed (GPS-leveling diff.) and computed (gravimetric)<br />

geoid heights for Ψ 0 = 1.25 0 for different degrees of modification (P)<br />

Fig.4 Comparison of observed (GPS-leveling diff.) and computed (gravimetric)<br />

geoid heights for Ψ 0 = 1.5 0 for different degrees of modification (P)<br />

Fig.5 Comparison of observed (GPS-leveling diff.) and computed (gravimetric)<br />

geoid heights for Ψ 0 = 2 0 for different degrees of modification (P)<br />

low degree range gives better solutions.<br />

Considering these facts we testified the<br />

results starting with P=40 and allowed<br />

to vary in the step of 10 to evaluate the<br />

change in performance. The RMS error<br />

was taken as the standard parameter in<br />

order to select the optimum degree of<br />

modification. Fig. 7 clearly indicates<br />

that RMS error of the Least square fit<br />

is lowest for the solution derived using<br />

P=70 as degree of kernel modification.<br />

The above illustrations gives an<br />

overview of the procedure to be<br />

adopted while deriving the optimum<br />

solution for gravimetric geoid. The<br />

GPS–leveling observations are<br />

of great help in this process and<br />

without it the quality assessment<br />

of gravimetric geoid solution can<br />

not be made with authenticity.<br />

Conclusion<br />

Rather than presenting simply the<br />

requirements of GPS – levelling data<br />

only for comparison purpose this<br />

study has focussed its importance<br />

in deriving an optimized solution of<br />

gravimetric geoid. Wonge and Gore<br />

modification approach was examined<br />

and its performance was evaluated by<br />

changing size of cap radius and degree<br />

of modifications which is an arguably<br />

more informative exercise rather than<br />

making the geoid determination as<br />

routine computation. The problems<br />

that may be encountered when<br />

practically applying the modified<br />

kernels have been described. The<br />

case study has practically proved the<br />

optimisation procedure to be followed<br />

and importance of GPS–leveling data<br />

in this process. However, because of<br />

the pecularities of local gravity data<br />

error characteristics the modifications<br />

approach and its parameter might<br />

vary from region to region in practical<br />

gravimetric geoid computation<br />

References<br />

1. Evans, J.D., Featherstone, W.E.<br />

2000. Improved convergence rates<br />

for truncation error in gravimetric<br />

geoid determination, Journal of<br />

Geodesy 74 (2), 239 – 248.<br />

2. Featherstone. W.E., 2003, Software<br />

for computing five existing types<br />

of deterministically modified<br />

integration kernel for gravimetric<br />

geoid determination. Computers<br />

and Geosciences, 29, 183-193.<br />

3. Heck. B., Grüninger, W.,1987.<br />

Modification of Stoke’s integral<br />

formula by combining two<br />

classical approaches. Proceedings<br />

of the XIX General Assembly<br />

of the International Union<br />

of Geodesy and Geophysics,<br />

Vol. 2. Vancouver, Canada.<br />

4. Heiskanen, W.H., Moritz, H., 1967.<br />

Physical Geodesy. W.H. Freeman &<br />

Co.., San Francisco, CA, 364 pp.<br />

5. Lemoine, F.G., Kenyon S.C.,<br />

April 2006 11

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