A Solution for the Sun-Mars Ration Using Mariner IV Doppler Tracking Data

1967 ◽  
Vol 72 ◽  
pp. 1292 ◽  
Author(s):  
G. W. Null
1997 ◽  
Vol 45 (4) ◽  
pp. 451-469
Author(s):  
George W. Davis ◽  
John C. Ries ◽  
Byron D. Tapley

1980 ◽  
Vol 56 ◽  
pp. 325-328
Author(s):  
William H. Michael ◽  
George M. Kelly

AbstractDynamical constants and other fundamental reference parameters for Mars have been derived from analyses of Viking lander ranging and Doppler tracking data covering a time span of nearly four years. Precise values have been obtained for the coordinates of the spin axis and for the rotation rate, suggesting that these Viking-derived values are definitive and are suitable for adoption by the IAU. Preliminary results have been obtained for a small seasonal variation in the rotation rate, and progress has been made toward a direct determination of the precession constant.


1995 ◽  
Vol 16 (12) ◽  
pp. 89-92
Author(s):  
F.J. Lerch ◽  
C.E. Doll ◽  
J.A. Marshall ◽  
S.B. Luthcke ◽  
R.G. Williamson ◽  
...  

2005 ◽  
Vol 13 ◽  
pp. 921-921 ◽  
Author(s):  
Guangyu Li ◽  
Wei-Tou Ni ◽  
Chien-Jen Tang

ASTROD I with one spacecraft ranging optically with ground stations is a first step for a full ASTROD (Astrodynamical Space Test of Relativity using Optical Devices) mission. The goals are testing relativity with the relativistic parameter γ measured to 10~7, measuring solar-system parameters more precisely, and improving the present-day sensitivity for gravitational wave detection using Doppler tracking by radio waves. In this paper, we present the mission concept and the orbit design for ASTROD I with an emphasis on Venus flybys. The spacecraft is to be launched into an inner solar orbit with initial period about 290 days to encounter Venus twice to receive gravity-assistance for achieving shorter period (165 days or less) to reach the other side of the Sun for a sooner measurement of Shapiro time delay. For a launch on June 17, 2010, after two encounters with Venus, the orbital period can be shortened to 165 days and the spacecraft orbit reaches inside Mercury orbit. After about 400 days from launch, the spacecraft will arrive at the other side of the Sun and the relativistic parameter γ can be determined to 0.1 ppm or better. A simulation of the accuracy for determining the relativistic parameters γ and β, and the solar quadrupole parameter J2 gives 10−7, 10−7 and 10−8 for their respective uncertainties. In this simulation, we assume a 10 ps timing accuracy and 10−13 m/s2(Hz)1/2 at frequency f ~ 100μHz inertial sensor/accelerometer noise. Other orbits separated by synodic periods of Venus can readily be found. We discuss the sensitivity and noise reduction requirements, the atmosphere transmission noise, timing noise, spacecraft environmental noise, test-mass sensor back-action, and test mass-spacecraft control-loop noise and stiffness. In the second Venus flyby, the ASTROD I could also be swung into an elliptic 360-day orbit and stay near opposite side of the Sun for many good measurements of the Shapiro time delays — 19 times in 10 years. This is an interesting alternative. In the two Venus flybys, Venus multiple moments can be determined very precisely. In this paper, we also review ASTROD and discuss its gravitational-wave sensitivities.


Author(s):  
Eric Smith ◽  
Patrick Morinelli ◽  
Michael Moreau ◽  
Dennis Woodfork ◽  
Rivers Lamb

1999 ◽  
Vol 172 ◽  
pp. 417-418
Author(s):  
Sebastian Bouquillon ◽  
Jean Souchay

AbstractFollowing efforts to construct an accurate modelisation of Mars rotation starting from canonical equations in an Hamiltonian theoretical frame (Bouquillon and Souchay, 1996), we use recent results from radio tracking data of the Mars Pathfinder mission (Folkner et al., 1997) to modelize in the best way the motion of precession and nutation of the planet. A complete set of coefficients related to these two motions is presented, including the main effect due to the Sun and also those due to the two satellites Phobos and Deimos as well as to the planets. Morever, Oppolzer terms are calculated and included.


2019 ◽  
Vol 29 (04) ◽  
pp. 1940002 ◽  
Author(s):  
Toshikazu Ebisuzaki ◽  
Hidetoshi Katori ◽  
Jun’ichiro Makino ◽  
Atsushi Noda ◽  
Hisaaki Shinkai ◽  
...  

The new technique of measuring frequency by optical lattice clocks now approaches to the relative precision of [Formula: see text]. We propose to place such precise clocks in space and to use Doppler tracking method for detecting low-frequency gravitational wave below 1[Formula: see text]Hz. Our idea is to locate three spacecrafts at one A.U. distance (say at L1, L4 and L5 of the Sun–Earth orbit), and apply the Doppler tracking method by communicating “the time” each other. Applying the current available technologies, we obtain the sensitivity for gravitational wave with third- or fourth-order improvement ([Formula: see text] or [Formula: see text] level in [Formula: see text]–[Formula: see text][Formula: see text]Hz) than that of Cassini spacecraft in 2001. This sensitivity enables us to observe black hole (BH) mergers of their mass greater than [Formula: see text] in the cosmological scale. Based on the hierarchical growth model of BHs in galaxies, we estimate the event rate of detection will be 20–50 a year. We nickname “INO” (Interplanetary Network of Optical Lattice Clocks) for this system, named after Tadataka Ino (1745–1818), a Japanese astronomer, cartographer, and geodesist.


1986 ◽  
Vol 34 (4) ◽  
pp. 984-990 ◽  
Author(s):  
T. Piran ◽  
E. Reiter ◽  
W. G. Unruh ◽  
R. F. C. Vessot

2002 ◽  
Vol 29 (8) ◽  
pp. 72-1-72-3 ◽  
Author(s):  
Romain Garmier ◽  
Jean-Pierre Barriot ◽  
Alexander S. Konopliv ◽  
Donald K. Yeomans

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