Data of Core Angular Momentum Changes




Author(s) : Dale Boggs

Affiliation : Jet Propulsion Laboratory Caltech, Pasadena, California.

Sampling time interval : 2.5 years

Data unit : Excess length of day in milliseconds over standard day of 86400 seconds

Modelling hypotheses :

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 :

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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