Malaysia precise geoid
(MyGEOID)
AHMAD FAUZI NORDIN, SAMAD HJ. ABU, CHANG
LENG HUA & SOEB NORDIN
The
Malaysian geoid project (MyGEOID) is unique
where the whole country is covered by with
dense airborne gravity with the aim to make
the best possible national geoid model
GPS
infrastructures that have been established in
Malaysia are mainly served as a ground control
stations for cadastral and mapping purposes. Another
element that has not been utilised is the height
component due to its low accuracy. Conventional
levelling is still the preferred method by the
land surveyors to determine the stations orthometric
height (H) with a proven accuracy. Therefore,
Department of Survey and Mapping Malaysia (DSMM)
has embarked the Airborne Gravity Survey, with
one of the objectives is to compute the local
precise geoid for Malaysia within centimeter level
of accuracy. With the availability of the precise
geoid, the “missing” element of GPS
system is solved.
The Malaysian geoid project (MyGEOID) is unique
where the whole country is covered by with dense
airborne gravity, with the aim to make the best
possible national geoid model. The basic underlying
survey and computation work of the Malaysian geoid
project was done by Geodynamics Dept. of the Danish
National Survey and Cadastre (KMS; since Jan 1
part of the Danish National Space Center) in cooperation
with JUPEM. With the new data the geoid models
are expected to be much improved over earlier
models (Kadir et al. 1998).
Objectives
The main
objective of the Malaysian geoid model (MyGEOID)
is to be able to compute orthometric heights H
that refer to the national geodetic vertical datum
(NGVD). Mathematically, there is a simple relation
between the two reference systems (neglecting
the defl ection of the vertical and the curvature
of the plumb line):
where,
hGPS is the GPS height above the ellipsoid and
N the geoid seperation. In the above equation
it is important to realize that H refers to a
local vertical datum, hGPS refers to a geocentric
system (ITRF/ WGS84), to which the computed (gravimetric)
geoid also usually refers.
In practice, the expression shows
the possibility of using GPS leveling technique,
knowing the geoidal height N, the orthometric
height H can be calculated from ellipsoidal height
h. Deriving orthometric height using this technique
with certain level of accuracy, could replace
conventional spirit leveling and therefore make
the levelling procedures cheaper and faster.
The existence of datum bias (differences between
geoid and local mean sea level) will not gives
satisfactory results if based on the above formula.
In order to overcome this problem, fi tting the
gravimetric geoid onto the local mean sea level
(NGVD) will minimize the effect of datum biases.
Gravity data acquisition
and processing
Gravity
data
The Malaysian
airborne gravity survey was done on a 5 km line
spacing, covering mostly Sabah and Sarawak in
2002 and Peninsular Malaysia in 2003. The airborne
gravity data system used was based on the Danish
National Space Center (DNSC)/University of Bergen
system, used extensively for Arctic gravity field
mapping. The system is based on differential GPS
for positioning, velocity and vertical accelerations,
with gravity sensed by a modifi ed marine Lacoste
and Romberg gravimeter. The system has a general
accuracy better than 2 mgal at 5 km resolution.
For the Malaysia airborne survey, the system was
installed in a An- 38 aircraft (Figure 1, below),
and the aircraft turned out to be very suitable
for the airborne survey, with accuracies estimated
from crossovers well below 2 mgal r.m.s.
The airborne gravity survey was flown at different
elevations, as topographic conditions permitted,
see Figure 2 and 3. The data were therefore required
to be downward continued to the surface, before
applying the Stokes formula gravity to geoid transformation.
The downward continuation was done by least-squares
collocation using the planar logarithmic covariance
model (Forsberg, 1987), using all available gravity
data in the process (airborne, surface, marine
and satellite altimetry gravity data). The Stokes’
integration was implemented by spherical FFT methods
(Forsberg and Sideris, 1993).
The existing surface gravity data coverage was
only of signifi cance in Peninsular Malaysia (Figure
4). Here the relatively dense surface gravity
data coverage in the lowlands will strengthen
the geoid compared to the situation in Sabah and
Sarawak, where a minimum gravity data was available.
Gravimetric
GEOID computation
For the
Malaysian project new GRACE satellite data combination
models were used (GGM01C). This model is a combination
model to degree 180 based on 1° mean anomalies,
essentially derived from the same terrestrial
data as EGM96, but having superior new satellite
information (GGM01S) at the lower harmonic degrees.
A third data source for the geoid determination
is digital terrain models (DEM’s), which
provide details of the gravity field variations
in mountainous areas (the mass of the mountains
can change the geoid by several 10’s of
cm locally). The handling of digital terrain models
is done by analytical prism integration assuming
known rock density (Forsberg, 1984). The new satellite
data SRTM was used together with JUPEM DEM’s
for this purpose.
With the
data from spherical harmonic models, local or
airborne gravity,
and DEM’s, the (gravimetric) geoid is constructed
by removerestore techniques as a sum
The summary
of gravity data used in the gravimetric geoid
computation are tabulated in Table 1 and the computed
geoid models for Sabah and Sarawak (EMG03C) as
in Figure 5 and Peninsular Geoid model (WMG03A)
as in Figure 6.