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911.
多点系泊下后弯管波力发电浮体模型试验研究 总被引:1,自引:5,他引:1
在大型造波水池中,对最佳后弯管浮体模型3-3,进行了多点系泊下浮体模型试验研究。测定了该模型在不同系泊条件下,气室平均输出气流功率随波周期的变化曲线NA-T,最大锚泊力与入射波高之比随波周期的变化曲线Fmax/Ho-T和最大纵荡距离与入射波高Ho之比随波周期变化曲线Xmax/Ho-T。选定L型链三点系泊为最佳系泊方案。进行了不同喷嘴比的性能试验和不类来波方向的试验,测定了浮体波能转换性能、最大锚泊力、最大纵荡距离随来波方向的变化。 相似文献
912.
The right-lateral Blanco Transform Fault Zone (BTFZ) offsets the Gorda and the Juan de Fuca Ridges along a 350 km long complex zone of ridges and right-stepping depressions. The overall geometry of the BTFZ is similar to several other oceanic transform fault zones located along the East Pacific Rise (e.g., Siquieros) and to divergent wrench faults on continents; i.e., long strike-slip master faults offset by extensional basins. These depressions have formed over the past 5 Ma as the result of continual reorientation of the BTFZ in response to changes in plate motion. The central depression (Cascadia Depression) is flanked by symmetrically distributed, inward-facing back-tilted fault blocks. It is probably a short seafloor spreading center that has been operating since about 5 Ma, when a southward propagating rift failed to kill the last remnant of a ridge segment. The Gorda Depression on the eastern end of the BTFZ may have initially formed as the result of a similar occurrence involving a northward propagating rift on the Gorda ridge system. Several of the smaller basins (East Blanco, Surveyor and Gorda) morphologically appear to be oceanic analogues of continental pull-apart basins. This would imply diffuse extension rather than the discrete neovolcanic zone associated with a typical seafloor spreading center. The basins along the western half of the BTFZ have probably formed within the last few hundred thousands years, possibly as the result of a minor change in the Juan de Fuca/Pacific relative motion. 相似文献
913.
914.
915.
论东海陆架盆地玉泉运动 总被引:1,自引:0,他引:1
据地质及地球物理勘探资料,并结合周围邻近盆地的对比研究后提出:(1)目前确定的新玉泉运动,其影响比前人描述的轻微得多;(2)以前所确定的原(老)玉泉运动的活动强度比新玉泉运动强烈得多,不应将原(老)玉泉运动取消,而应将新、老玉泉运动的间隔期视为构造变革过渡期。 相似文献
916.
New Derivation of Ordinary Differential Equations for Transient Free-Surface Green Functions 总被引:3,自引:0,他引:3
DUAN Wenyang DAI Yishan 《中国海洋工程》2001,(4):499-508
Based on the Laplace transform, a direct derivation of the ordinary differential equations for the three-dimensional transient free-surface Green function in marine hydrodynamics is presented. The results for the 3D Green function and all its spatial derivatives are a set of fourth-order ordinary differential equations, which are identical with that of Clement (1998). All of these results may be used to accelerate numerical computation for the time-domain boundary element method in marine hydrodynamics. 相似文献
917.
Beng-Chun Lee Li-Chung Wu Dong-Jiing Doong Chia Chuen Kao 《Marine Geophysical Researches》2007,28(3):183-190
We here investigate the frequency and intensity of oscillations in oceanographic data within intraseasonal time scales using
spectral analysis of surface wind and wave time-series data collected at off-island weather stations or moored buoys around
Taiwan. Data from marine weather stations were used to trace atmospheric conditions, while we used buoy data to examine sea
states. The spectra and wavelet scalogram of the wind fields revealed oscillations with a period of around 20–33 days, and
the energy density of the wind field at the off-island stations was stronger than that at the data buoy stations. However,
the wavelet scalogram of the wave height measured at the buoy stations was stronger than its associated wind field. This long-period
oscillation is consistent with the wavelet scalogram of the wind field calculated from the off-island weather stations. About
20–33 day oscillations exist within intraseasonal variations, which are closely linked to the atmospheric environment and
to wind and ocean wave fields. Oscillations with a period of 5–10 days are a pronounced feature over northeastern Taiwan waters
during the winter season and can be interpreted as the wave pattern following synoptic weather systems. 相似文献
918.
The Kane Fracture Zone probably is better covered by geophysical survey data, acquired both by design and incidentally, than
any other fracture zone in the North Atlantic Ocean. We have used this data to map the basement morphology of the fracture
zone and the adjacent crust for nearly 5700 km, from near Cape Hatteras to the middle of the Mesozoic magnetic anomalies west
of Cap Blanc, northwest Africa. We use the trends of the Kane transform valley and its inactive fracture valley to determine
the record of plate-motion changes, and we interpret the basement structural data to examine how the Kane transform evolved
in response to changes in plate motion. Prior to about 133 Ma the Kane was a small-offset transform and its fracture valley
is structurally expressed only as a shallow ( < 0.5 km) trough. In younger crust, the offset may have increased to as much
as 190 km (present offset 150 km) and the fracture valley typically is up to 1.2 km deep. This part of the fracture valley
records significant changes in direction of relative plate motion (5°–30°) near 102 Ma, 92 Ma, 59 Ma, 22 Ma, and 17 Ma. Each
change corresponds to a major reorganization of plate boundaries in areas around the Atlantic, and the fracture-zone orientation
appears to be a sensitive recorder of these events.
The Kane transform has exhibited characteristic responses to changes in relative plate motion. Counterclockwise plate-motion
changes put the left-lateral transform offset into extension, and the response was for ridge tips at the ridge-transform intersections
to propagate across the transform valley and against the truncating lithosphere. Heating of this lithosphere appears to have
produced uplift and formation of a well developed transverse ridge that bounds the inactive fracture valley on its older side.
The propagating ridge tips also rotated toward the transform fault in response to the local stress field, forming prominent
hooked ridges that now extend into or across the inactive fracture valley. Clockwise (compressional) changes in relative plate
motion produced none of these features, and the resulting fracture valleys typically have a wide-V shape.
The Kane transform experienced severe adaptions to the changes in relative plate motion at about 102 Ma (compressional shift)
and 92 Ma (extensional shift), and new transform faults were formed in crust outside the contemporary transform valley. Subsequently,
the transform offset has been smaller and the rates of change in plate motion have been more gradual, so transform-fault adjustment
has been contained within the transform valley. The fracture-valley structure formed during extensional and compressional
changes in relative plate motion can be decidedly asymmetrical in conjugate limbs of the fracture zone. This asymmetry appears
to be related to the ‘absolute’ motion of the plate boundary with respect to the asthenosphere. 相似文献
919.
A plane strain analysis based on the generalized Biot's equation is utilized to investigate the wave-induced response of a poro-elastic seabed with variable shear modulus.By employing integral transform and Frobenius methods,the transient and steady solutions for the wave-induced pore water pressure,effective stresses and displacements are analytically derived in detail.Verification is available through the reduction to the simple case of homogeneous seabed.The numerical results indicate that the inclusion of variable shear modulus significantly affects the wave-induced seabed response. 相似文献
920.