The zonal toroidal t_1^0 and t_3^0 components of a fully time dependent
geostrophic flow constructed under the frozen flux hypothesis are used to
estimate the core angular momentum (CAM) using the hypothesis of Jault Gire and
Le Mouel (1988). The CAM is then transformed into an equivalent change in
the length of the day as seen on the solid earth by conservation of
angular momentum. The predictions only give relative changes in the lod,
therefore an arbitrary offset should be chosen in order that the
predictions agree reasonably well with the lod series from astronomical
observations. A value of 3.25 milliseconds has been added to the predictions to
give the values presented here.
Description of the data used for model computation :
The magnetic field and its rate of change at the core-mantle interface was computed
at 2.5 year intervals from
field model ufm1 of Bloxham & Jackson (1992)
References to be mentioned when data are used :
R. Hide, D. H.
Boggs and J. O. Dickey, "Angular Momentum fluctuations within the Earth's
liquid core and torsional oscillations of the core-mantle system", Geophys.
J. Int. 143, 777-786, 2000.
Related references :
1840 | -8.5661 |
1842.5 | -9.048 |
1845 | -9.028 |
1847.5 | -8.676 |
1850 | -8.961 |
1852.5 | -8.476 |
1855 | -7.733 |
1857.5 | -7.7303 |
1860 | -7.060 |
1862.5 | -5.933 |
1865 | -5.920 |
1867.5 | -5.296 |
1870 | -4.297 |
1872.5 | -4.555 |
1875 | -3.994 |
1877.5 | -2.979 |
1880 | -3.197 |
1882.5 | -2.574 |
1885 | -1.554 |
1887.5 | -1.840 |
1890 | -1.819 |
1892.5 | -1.565 |
1895 | -1.981 |
1897.5 | -1.386 |
1900 | -0.495 |
1902.5 | -0.540 |
1905 | -0.823 |
1907.5 | -1.5650 |
1910 | -2.7578 |
1912.5 | -3.6481 |
1915 | -4.2847 |
1917.5 | -4.6803 |
1920 | -5.4042 |
1922.5 | -5.8092 |
1925 | -6.0432 |
1927.5 | -6.3627 |
1930 | -6.5348 |
1932.5 | -6.3271 |
1935 | -5.8398 |
1937.5 | -5.8491 |
1940 | -5.8493 |
1942.5 | -5.7387 |
1945 | -5.3583 |
1947.5 | -5.5345 |
1950 | -5.5270 |
1952.5 | -5.3597 |
1955 | -6.0454 |
1957.5 | -5.9644 |
1960 | -5.3984 |
1962.5 | -5.2508 |
1965 | -4.3351 |
1967.5 | -3.2817 |
1970 | -3.1235 |
1972.5 | -2.6982 |
1975 | -2.5018 |
1977.5 | -3.7217 |
1980 | -4.0370 |
1982.5 | -3.3787 |
1985 | -4.177 |
1987.5 | -4.8577 |