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  • 1
    Call number: MOP 25538
    In: Verhandelingen
    Type of Medium: Monograph available for loan
    Pages: 21 S.
    Series Statement: Verhandelingen / Koninklijk Magnetisch en Meteorologisch Observatorium te Batavia 29
    Location: MOP - must be ordered
    Branch Library: GFZ Library
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  • 2
    Call number: MOP 25541
    In: Verhandelingen
    Type of Medium: Monograph available for loan
    Pages: 20 S.
    Series Statement: Verhandelingen / Koninklijk Magnetisch en Meteorologisch Observatorium te Batavia 32
    Location: MOP - must be ordered
    Branch Library: GFZ Library
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  • 3
    Call number: MOP 25539
    In: Verhandelingen
    Type of Medium: Monograph available for loan
    Pages: 28 S.
    Series Statement: Verhandelingen / Koninklijk Magnetisch en Meteorologisch Observatorium te Batavia 30
    Location: MOP - must be ordered
    Branch Library: GFZ Library
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  • 4
    Call number: MOP 25544
    In: Verhandelingen
    Type of Medium: Monograph available for loan
    Pages: 14 S.
    Series Statement: Verhandelingen / Koninklijk Magnetisch en Meteorologisch Observatorium te Batavia 36
    Location: MOP - must be ordered
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  • 5
    Monograph available for loan
    Monograph available for loan
    Soerabaia : Van Ingen
    Associated volumes
    Call number: MOP 25542
    In: Verhandelingen
    Type of Medium: Monograph available for loan
    Pages: 20 S.
    Series Statement: Verhandelingen / Koninklijk Magnetisch en Meteorologisch Observatorium te Batavia 33
    Location: MOP - must be ordered
    Branch Library: GFZ Library
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  • 6
    Monograph available for loan
    Monograph available for loan
    Soerabaja
    Associated volumes
    Call number: MOP 25545
    In: Verhandelingen
    Type of Medium: Monograph available for loan
    Pages: 16 S.
    Series Statement: Verhandelingen / Koninklijk Magnetisch en Meteorologisch Observatorium te Batavia 35
    Location: MOP - must be ordered
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  • 7
    Electronic Resource
    Electronic Resource
    Springer
    Pure and applied geophysics 44 (1959), S. 287-295 
    ISSN: 1420-9136
    Source: Springer Online Journal Archives 1860-2000
    Topics: Geosciences , Physics
    Notes: Summary The Southern Oscillation in air pressure may be described primarily as an air pressure balance whose scales are centred near Djakarta (Indonesia) and near Easter Island (South Pacific Ocean) respectively. A synoptic station was established at Easter Island July 1, 1949. 1) The 8 twelve-monthly air pressure values of Djakarta and Easter Island from the period July 1949 up to July 1957 have been correlated with the simultaneous air pressure values at 289 stations throughout the world; 2) The 7 twelve-monthly air pressure values of Djakarta and Easter Island from the period July 1949 up to July 1956 have been correlated with the simultaneous air pressure values at 65 grid points in North Asia and from the period July 1950 up to July 1957 with simultaneous air pressure values at 32 grid points in Africa; 3) At least 5 twelve-monthly air pressure values of Djakarta and Easter Island have been correlated with simultaneous air pressure values at 159 grid points between latitudes 20° and 60° S (Southern Hemisphere Project, Weather Bureau, Pretoria). The latter coefficients obtained, being less reliable, have been used only indicatively. The 545 correlation coefficients have been plotted on world charts and isopleths of the correlation coefficients with the values −0.9,; −0.7; −0.4; 0; +0.4; +0.7 and +0.9 have been drawn (Fig. 1 and 2). The patterns of the isopleths on both maps are very much alike. This is due, of course, to the fact that the coefficient of correlation between Djakarta and Easter Island air pressure deviations reaches a value as high as −0.93. From these pictures may be inferred that the Southern Oscillation acts for the greater part as a stationary wave and for the rest as a progressive wave. Another prominent feature of the Southern Oscillation, shown by the pictures, is that the Easter Island scale is meridionally developed, whereas the Djakarta scale is mainly zonally developed, especially along the equator. It is shown to be very probable that the arctic and antarctic regions both cooperate with the Djakarta region, thus stressing an undeniable overall zonal symmetry of the two patterns. A first impression is obtained of the kind of encroachment of the antarctic circulation on the Southern Oscillation. The well detailed patterns in the northern moderate and high latitudes call up the idea of the planetary waves in the zonal current which normally flows through these latitudes and the question is raised whether blocking action is stimulated when the Southern Oscillation is well developped. Similar indications are obtained from the still rather provisional and rough patterns in the southern moderate and high latitudes.
    Type of Medium: Electronic Resource
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  • 8
    Electronic Resource
    Electronic Resource
    Springer
    Pure and applied geophysics 53 (1962), S. 198-207 
    ISSN: 1420-9136
    Source: Springer Online Journal Archives 1860-2000
    Topics: Geosciences , Physics
    Notes: Summary The barometric pressure curve at Jakarta is presumed to consist of two components. The first is the basic air pressure, which shows a relaxation oscillation during a periodt 1. The value oft 1 may differ for the successive periods. The second component is the Southern Oscillation proper, which is superimposed on the basic air pressure. This system of two kinds of oscillations may be expressed in the form of a differential equation. The solution of the equation depends on the value of a certain constant. If the value is greater than zero, the solution shows a S.O. the amplitude and period of oscillation of which decreases in time. If the value is less than zero, the solution shows a S.O. the amplitude of which decreases in time and the period of oscillation of which increases in time. As an example of the first contingency the values of the constants occurring in the solution were determined for the period 1868–1876 so that a good approximation to the existing air pressure curve could be attained. It was possible to establish a relationship between the basic air pressure level and the period of oscillation of the S.O. The air pressure curve at Jakarta during the years 1876–1884 was reconstructed from this relationship. The two trains of 3-year waves in 1885–1891 and 1896–1905 may be regarded as an example of the second contingency.
    Type of Medium: Electronic Resource
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  • 9
    Electronic Resource
    Electronic Resource
    Springer
    Pure and applied geophysics 46 (1960), S. 329-351 
    ISSN: 1420-9136
    Source: Springer Online Journal Archives 1860-2000
    Topics: Geosciences , Physics
    Notes: Summary The eight successive twelve-monthly airpressure values of Djakarta and Ponta Delgada from July 1949 up to July 1957 have been correlated with the simultaneous airpressure values at 292 meteorological stations and 256 grid points throughout the world. The 548 correlation coefficients have been plotted on world charts and isocorrelates for the values −0.9, −0.7, −0.4, 0.0, +0.4, +0.7 and +0.9 have been drawn (Figs. 1 and 2). The same has been done for the series of eight years January 1931 up to January 1939 with 351 meteorological stations and 259 grid points (Figs. 4 and 5). For both series of eight years the length of the period and the ratio noise-signal of the Southern Oscillation as well as the North Atlantic Oscillation have been determined. From these charts and these determinations the authors drew the following conclusions. 1) 1 July 1949–1 July 1957. The average length of the period of the S. O. amounts to 29.8 months, while the amplitude of the S.O. exceeds the noise amplitude by 33 per cent in its own region. The average length of the period of the N.A.O. amounts to 20.8 months, while its amplitude is only half the noise amplitude in its own region. The amplitude of the S.O. even exceeds the amplitude of the N.A.O. by 24 per cent in the North Atlantic Ocean. Hence the S.O. is well developed, whereas the N.A.O. is not. 2) 1 January 1931–1 January 1939. The average length of the period of the N.A.O. amounts to 20.8 months, while its amplitude exceeds the noise amplitude by more than 20 per cent. The average length of the period of the S.O. also amounts to 20.8 months, whereas the noise amplitude is 1.09 times the amplitude of the S.O. Hence the N.A.O. is well developed, whereas the S.O. is not. In this case the N.A.O. is generating a forced oscillation in the region of the S.O. The correlation patterns show prevalence of a summer-circulation type during 1931–1939 and of a winter-circulation type during 1949–1957 on both hemispheres. Arguments are gathered for the excitation and ruling of the S.O. by a relaxation oscillation (Fig. 8). The relaxation apparently occurs after long persistence of an excessive pressure difference between the Easter Island High and the Djakarta Low, and results in a sudden large increase of the amplitude and of the wave length of the S.O. Thereafter both amplitude and wave length of the S.O. gradually decrease. The general atmospheric and hydrospheric circulation in the South Pacific Ocean are accelerated until the next relaxation. The generation of regular S.O. wave trains as occurred in the last two decades of the 19th century and the first decade of the 20th century requires a special condition. Finally the relations between the fluctuations of solar activity and the S.O. and the relations between the S.O. and the weather even in moderate and high latitudes are discussed.
    Type of Medium: Electronic Resource
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  • 10
    Electronic Resource
    Electronic Resource
    Springer
    Pure and applied geophysics 37 (1957), S. 309-317 
    ISSN: 1420-9136
    Source: Springer Online Journal Archives 1860-2000
    Topics: Geosciences , Physics
    Notes: Summary Characteristic features of long-periodic oscillations in the general atmospheric circulation may be deduced from the correlation existing between the monthly, the three-monthly, the six-monthly and the twelve-monthly figures of the barometric pressure at two distant stations and from the autocorrelation of the same figures at each station. It is shown that the monthly figures of the barometric pressure at Easter Island and those at Djakarta during the six years 1950–1955 have, when plotted as a function of time, one oscillation in common, whereas further these figures have both their own rhythms and their own noise. The period of the common oscillation is 28.6 months, while the phase difference between both stations amounts to 180°. The r.m.s. value of the noise is 0.76 times the value of the amplitude of the oscillation. The rhythms differ in wave length, amplitude and phase. It is also shown that the monthly figures of the barometric pressure at Ponta Delgada and those at Stykkisholm have, when plotted as a function of time, a whole spectrum of oscillations jointly, while all oscillations have the same phase difference (238°) between both stations. These features are deduced from observations during 40 years (1896–1915 and 1921–1940). If yearly figures are used instead of monthly ones, then the greater part of the spectrum of oscillations is smoothed away and only a few common oscillations are left. The first common oscillation has a wave length of 26.5 months and the second one has a wave length of 38.7 months.
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