|
|
frequency
shift. This is referred to as the equi-frequency
geoid (Shen 1998). Now, suppose the light signal
emitter E is located in a satellite, and two light
signal receivers at P and Q receive the light
signals coming from E corresponding to an emitting
time t (Cf. Fig.2). Further suppose the received
signals’ frequencies corresponding to time
t are recorded by receivers at P and Q in some
way, respectively, i.e., fP and fQ corresponding
to time t are recorded by receivers at P and Q,
respectively. Note that the time at which the
signal is received by P is generally different
from that by Q. By comparing the received frequencies
fP and fQ it could be determined the geopotential
difference ?WPQ = WQ – WP (Shen et al.,
1993), which is just given by Eq. (1).
By the above mentioned way, the geopotential on
the Earth’s whole surface could be determined
based on the geopotential frequency shift approach
by receiving the light signals emitted by satellites.
Once the geopotential W on the Earth’s surface
is determined, the potential field V outside the
Earth could be determined, and as a result, the
geoid could be more precisely determined.
The emitter could be a distant stable star. The
receivers at P and Q could be designed in such
a way that the received light signals might be
recorded on diskettes at P and Q in details. Then,
comparing the recorded diskettes at a centre process
system. In this way, the frequency shift information
between P and Q might be drawn out.
In the case that the emitter is located on the
Earth’s surface, the potential difference
between the two points P and Q could be also directly
determined based on the same principle, as long
as the the receivers at these two points could
simultaneously receive the light signals emitted
by the emitter.
It is noted that the accuracy for determining
the potential difference by using the geopotential
frequency shift approach is becoming more and
more prospective for the goal of determining the
centimeter-geoid, which is mainly depending on
the frequency stability of the receiver. More
than 10 years ago, the frequency stability was
around 10-14, which is very poor for determining
the geoid with an adequate accuracy. At present
however, the frequency stability is around 10-15
- 10-16 (HMC Project 2005), which corresponds
to the height variation about 1 m. In the next
ten years, it is prospective that the frequency
stability 10-17 - 10-18 could be achieved, which
corresponds to the height variation 1cm.
The great advantage by using the geopotential
frequency shift approach lies in that a uni?ed
global datum system could be established: two
receivers located at two datum points A and B
which belong to two separated continents could
simultaneously receive the signals emitted by
a satellite source emitter, and consequently the
frequency shift between A and B is determined;
then, based on the geopotential frequency shift
equation the geopotential difference between A
and B is determined.
With satellite technique (e.g. CHAMP mission,
Cf. Gerlach 2003), the potential on the satellite
surface could be determined, and consequently
it could be determined the Earth’s could
be determined the Earth’s external potential
field, which is quite accurate for the long and
middle wave-length of the field, but not for the
short wave-length of the field.
The will-be launched GOCE system could provide
a 10 x 10 global gravity model with accuracy level
around 1cm. However, concerning a single datum
point A, the accuracy of the potential at A determined
based on the global gravity model is far from
centimeter level. To get more precise result,
local measurements (gravimetry and leveling) are
needed. Hence, with the goal of determining the
global centimeter-geoid, the connections between
different datum points located on different continents
should be precisely established, which might be
completed by geopotential frequency shift approach. |
| Acknowledgements |
This study
is funded in parts by Natural Science Foundation
China (No.40574004), and the Foundation of the
Key Lab. of Geospace Environment and Geodesy,
Ministry of Education China (03-04-13). |
| References |
Bjerhammar
A (1985) A relativistic geodesy. Royal Institute
of Technology, Geodesy Division, Stockholm. Gerlach
Ch., Földvary L., Svehla D., Gruber Th.,
Wermuth M., Sneeuw N., Frommknecht B., Oberndorfer
H., Peters Th., Rothacher M., Rummel R., Steigenberger
P. (2003) A CHAMP-only gravity field model from
kinematic orbits using the energy integral. Geophysical
Research Letters 30(20), 2037. Heiskanen W.A.,
Moritz H. (1967) Physical Geodesy. Freeman and
Company, San Francisco. HMC Project (2005) http://cfawww.
harvard.edu/hmc/
Katila T., Riski Q. (1981) Measurement of the
interaction between electromagnetic radiation
and gravitational field using 67Zn Mössbauer
spectroscopy. Physics Letters, 83A: 51-54.
Pound R.V., Snider J.L. (1965) Effect of gravity
on gamma radiation. Physical Review, 140(3B):
788-803.
Rummel R., Sansó F., van Gelderen M., Brovelli
M., Koop R., Miggliaccio
F., Schrama E., Sacerdote F. (1993)
Spherical harmonic analysis of satellite gradiometry.
Netherlands Geodetic Commission, Publications
on Geodesy, New Series No. 39
Shen W.B. (1998) Relativistic physical geodesy.
Habilitation Thesis, Graz Technical University,
Graz, Austria.
Shen W.B. (2004) The fictitious compress recuperation
method for gravitational potential. Geomatics
and Information Science of Wuhan University 29(8):
720-724
Shen W.B., Chao D.B., Jin B.R. (1993) On the relativistic
geoid. Bollettino di Geodesia e Scienze Affini,
52: 207-216.
Vessot R.F.C., Levine M.W., Mattison E.M., Blomberg
E.L., Hoffman T.E.,
Nystrom G.U., Farrel B.F., Decher R., Eby P.B.,
Baugher C.R., Watts J.W., Teuber D.L., Wills F.D.
(1980) Test of relativistic gravitation with a
space-borne hydrogen maser. Physical Review Letters,
45: 2081-2084.
Weinberg S. (1972) Gravitation and cosmology.
John Wiley & Sons, New York.
|
| December
2005 |
 |
W
B Shen
Department of Geophysics,
Wuhan University, Wuhan,
China |
| wbshen@sgg.whu.edu.cn |
|
|
| <<Previous... 2
of 2 |
| |
|
|