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81.
Summary The stress and strain fields in various earth models are studied under the assumption of an elastic mantle and the existence of thermal stresses which are proportional to the difference between the initial and present temperatures. The thermoelastic equilibrium equation for a 49-layered earth with spherical symmetry is integrated and programmed for various combinations of velocities, densities and temperatures. Results show that the strains in the upper mantle depend to a great extent on the thermal model. Central radial strain ranges from 5.2 to 7.3 per cent and the central pressure ranges between 3.1 and 3.7×1012 dynes/cm2 for all models. It is established that the thermal history of the earth could not have changedBullen's pressures by more than 0.4×1012 dynes/cm2.Contribution No. 1095, Division of Geological Sciences, California Institute of Technology, Pasadena, California. 相似文献
82.
Summary An explicit solution is obtained for the system of equations describing the spheroidal motion in a homogeneous, isotropic, gravitating, elastic medium possessing spherical symmetry. This solution is used to derive the Green's dyad for a homogeneous gravitating sphere. The Green's dyad is then employed to obtain the displacement field induced by tangential and tensile dislocations of arbitrary orientation and depth within the sphere.Notation
G
Gravitational constant
-
a
Radius of the earth
-
A
o
=4/3 G
-
Perturbation of the gravitational potential
-
Circular frequency
-
V
p
,V
s
Compressional and shear wave velocities
-
k
p
=/V
p
-
k
s
=/V
s
-
k
p
[(2.8)]
- ,
[(2.17)]
-
f
l
+
Spherical Bessel function of the first kind
-
f
l
–
Spherical Hankel function of the second kind
-
x
=r
-
y
=r
-
x
o
=r
o
-
y
o
=ro
-
x
=r k
s
-
y
=r k
p
-
x
o
=r
o
k
s
-
y
o
=r
o
k
p
-
=a
-
=a
-
[(5.17)]
-
m, l
相似文献
83.
Ari Shlanger 《Pure and Applied Geophysics》1959,43(1):23-35
Summary Earthquake shear waves with period around 12.2 min have been lately reported byM. Båth (1958), who suggests that these might be due to torsional vibrations of the whole mantle on some axis through the centre of the earth. An attempt has been made here to put forward a theory which accounts for such vibrations. The general elastokinetic equation for a heterogeneous isotropic medium is solved for a free spherical shell overlying a liquid core, and the solution is investigated for the first two modes. The frequency equation is solved for a shell and the limiting cases of a full sphere and an infinitely thin shell. Application is then made for various approximate mantle models, and periods are found which are in fair agreement with the observed. It is then shown that if the rigidity of the core is taken into consideration a closer agreement with the observed might be attained.
This research was supported by Eng.Herbert E. Linden of Beverly Hills, California. 相似文献
Zusammenfassung Seismische Transversalwellen mit einer Periode von rund 12.2 min sind neulich vonM. Båth (1958) beobachtet worden, der vermutet, dass sie Torsionsschwingungen des ganzen Erdmantels um eine Achse durch das Erdzentrum sind. Ein Versuch wird hier gemacht eine Theorie für solche Schwingungen zu entwickeln. Die allgemeine elastokinetische Gleichung für ein heterogenes, isotropisches Medium wird für eine freie, sphärische Schale über einem flüssigen Kern gelöst, und die Lösung wird für die zwei ersten Schwingungsformen untersucht. Die Frequenzgleichung wird für eine Schale und für die Grenzfälle einer ganzen Sphäre und einer unendlich dünnen Schale gelöst. Die Lösungen werden dann auf verschiedene, approximative Mantel-Modellen angewendet, und Perioden werden gefunden, die ziemlich gute Übereinstimmung mit der beobachteten Periode zeigen. Es wird danach gezeigt, dass, falls die Righeit des Erdkerns in Betracht gezogen wird, eine noch bessere Übereinstimmung mit der beobachteten Periode erreicht wird.
This research was supported by Eng.Herbert E. Linden of Beverly Hills, California. 相似文献
84.
Spatial interpolation of monthly climate data for Finland: comparing the performance of kriging and generalized additive models 总被引:2,自引:2,他引:0
Juha Aalto Pentti Pirinen Juha Heikkinen Ari Venäläinen 《Theoretical and Applied Climatology》2013,112(1-2):99-111
The Finnish Meteorological Institute has calculated statistics for the new reference period of 1981–2010. During this project, the grid size has been reduced from 10 to 1 km, the evaluation of the interpolation has been improved, and comparisons between different methods has been performed. The climate variables of interest were monthly mean temperature and mean precipitation, for which the spatial variability was explained using auxiliary information: mean elevation, sea percentage, and lake percentage. We compared three methods for spatial prediction: kriging with external drift (KED), generalized additive models (GAM), and GAM combined with residual kriging (GK). Every interpolation file now has attached statistical key figures describing the bias and the normality of the prediction error. According to the cross-validation results, GAM was the best method for predicting mean temperatures, with only very small differences relative to the other methods. For mean precipitation, KED produced the most accurate predictions, followed by GK. In both cases, there was notable seasonal variation in the statistical skill scores. For the new reference period and future interpolations, KED was chosen as the primary method due to its robustness and accuracy. 相似文献
85.
Ari Buchalter Raul Jimenez Marc Kamionkowski 《Monthly notices of the Royal Astronomical Society》2001,328(2):520-526
We predict the Tully–Fisher (TF) and surface-brightness–magnitude relations for disc galaxies at and discuss the origin of these scaling relations and their scatter. We find that both halo dynamics and the star formation history play important roles, and we show that the variation of the TF relation with redshift can be a potentially powerful discriminator of galaxy-formation models. In particular, the TF relation at high redshift might be used to break parameter degeneracies among galactosynthesis models at , as well as to constrain the redshift distribution of collapsing dark-matter haloes, the star formation history and baryon fraction in the disc and the distribution of halo spins. 相似文献
86.
87.
88.
Christoph Münkel Noora Eresmaa Janne Räsänen Ari Karppinen 《Boundary-Layer Meteorology》2007,124(1):117-128
The Vaisala ceilometers CT25K and CL31 are eye-safe single lens lidar systems reporting attenuated backscatter profiles; they
often operate 24 h a day in fully automated, hands-off operation mode. These profiles can be used for more than just cloud-base
height determination. In dry weather situations, there is a fairly good correlation between the ceilometer near-range backscatter
and in situ PM10 concentration readings. The comparison of mixing height values based on soundings and on ceilometer backscattering
profiles indicates that ceilometers are suitable instruments for determining the convective mixing height. Its enhanced optics
and electronics enables the CL31 ceilometer to detect fine boundary-layer structures whose counterparts are seen in temperature
profiles. 相似文献
89.
Nahum Arav Tom A. Barlow Ari Laor Wallace L. W. Sargent & Roger D. Blandford 《Monthly notices of the Royal Astronomical Society》1998,297(4):990-998
We search for a direct signature of discrete 'clouds' in the broad-line region (BLR) of the Seyfert galaxy NGC 4151. For this purpose we apply cross-correlation (CC) analysis to a high-resolution Keck spectrum of the galaxy. No such signature is found in the data. In order for cloud models to be compatible with this result, there must be at least ∼3×107 emitting clouds in the BLR, where the limit is based on simulation of a homogeneous cloud population. More realistic distributions increase the lower limit to above 108 . These numbers are an order-of-magnitude improvement on our previous limit from Mrk 335, where the improvement comes from higher signal-to-noise ratio (S/N), broader lines and refined simulations. Combined with the predicted upper limit for the number of emitting clouds in NGC 4151 (106 –107 ), the derived lower limit puts a strong constraint on the cloud scenario in the BLR of this object. Similar constraints can be placed on models where the emission originates in streams and sheets. Thus, this investigation suggests that the broad emission lines (BELs) in NGC 4151, and by extension in all AGNs, are not made of an ensemble of discrete independent emitters. 相似文献
90.
Ari Ben-Menahem Ezra Aboodi Rivka Schild 《Physics of the Earth and Planetary Interiors》1974,9(4):265-289
The source of the Assam earthquake of Aug. 15, 1950 is revealed from amplitude observations of surface and body waves at Pasadena, Tokyo and Bergen. Seiches' amplitudes in Norway, initial P motions throughout the world, aftershocks and landslides distribution, PP/P ratio at Tokyo, R/L ratio and directivity at Pasadena, are also used. The ensuing fault geometry and kinematics is consistent with the phenomenology of the event and the known geology of the source area. It is found that a progressive strike-slip rupture with velocity 3 km/sec took place on a fault of length 250 km and width 80 km striking 330–337° east of north and dipping 55–60° to ENE. The use of exact surface-wave theory and asymptotic body-wave theory which takes into account finiteness and absorption, rendered an average shear dislocation of 35 m. A three-dimensional theory for the excitation of seiches in lakes by the horizontal acceleration of surface waves was developed. It is confirmed that Love waves near Bergen generated seiches with peak amplitude up to 70 cm depending strongly on the width of the channel.It is believed that the earthquake was caused by a motion of the Asian plate relative to the eastern flank of the Indian plate where the NE Assam block is imparted a tendency of rotation with fracture lines being developed along its periphery.Comparison with other well-studied earthquakes shows that although the magnitude of the Assam event superseded that of all earthquakes since 1950, its potency U0dS (700,000 m × km2) was inferior to that of Alaska 1964 (1,560,000 m × km2) and Chile 1960 (1,020,000 m × km2). 相似文献