全文获取类型
收费全文 | 565篇 |
免费 | 66篇 |
国内免费 | 121篇 |
专业分类
测绘学 | 7篇 |
大气科学 | 219篇 |
地球物理 | 182篇 |
地质学 | 113篇 |
海洋学 | 178篇 |
天文学 | 4篇 |
综合类 | 15篇 |
自然地理 | 34篇 |
出版年
2024年 | 1篇 |
2023年 | 3篇 |
2022年 | 8篇 |
2021年 | 17篇 |
2020年 | 21篇 |
2019年 | 12篇 |
2018年 | 13篇 |
2017年 | 8篇 |
2016年 | 13篇 |
2015年 | 14篇 |
2014年 | 30篇 |
2013年 | 29篇 |
2012年 | 28篇 |
2011年 | 37篇 |
2010年 | 26篇 |
2009年 | 49篇 |
2008年 | 49篇 |
2007年 | 49篇 |
2006年 | 62篇 |
2005年 | 44篇 |
2004年 | 32篇 |
2003年 | 26篇 |
2002年 | 25篇 |
2001年 | 23篇 |
2000年 | 15篇 |
1999年 | 22篇 |
1998年 | 18篇 |
1997年 | 15篇 |
1996年 | 13篇 |
1995年 | 7篇 |
1994年 | 7篇 |
1993年 | 8篇 |
1992年 | 2篇 |
1991年 | 4篇 |
1990年 | 3篇 |
1989年 | 4篇 |
1988年 | 4篇 |
1987年 | 3篇 |
1986年 | 4篇 |
1985年 | 1篇 |
1983年 | 1篇 |
1977年 | 1篇 |
1954年 | 1篇 |
排序方式: 共有752条查询结果,搜索用时 343 毫秒
651.
S. Ramos Buarque H. Giordani G. Caniaux S. Planton 《Dynamics of Atmospheres and Oceans》2004,37(4):295-311
Ocean models depend strongly on surface fluxes. When computed from atmospheric models, fluxes are affected by spin-up, i.e. they increase (or decrease) with forecast length. Such behavior may bias ocean models. The European Centre for Medium Range Forecasts (ECMWF) 40-year re-analysis (ERA-40) has been used to quantify short-range spin-ups of radiative and turbulent heat fluxes. Fluxes are compared as differences between two runs with the same initialization time. This method allows flux analysis over short-range forecasts as a function of distance from the initialization time. Results indicate that (i) latent heat flux spin-up increases with time but levels off after 24 h; (ii) sensible and radiative flux spin-ups remain constant after 6 h; (iii) regional spin-up of turbulent fluxes are systematic and can be larger than 30% for sensible heat but never exceeds 15% for latent heat; (iv) spin-up depends upon the season. The same analysis has been carried out with the ECMWF 15-year re-analysis (ERA-15); spin-ups in ERA-40 have been generally smaller than those in ERA-15. 相似文献
652.
南海夏季风爆发前后海-气界面热交换特征 总被引:20,自引:1,他引:20
文中利用 2 0 0 0与 2 0 0 2年二次南海海 气通量观测资料和同期西沙站资料 ,研究了南海夏季风爆发前后海洋表面热收支变化特征。研究表明 :南海夏季风爆发前后 ,影响海面热收支变化的主要分量是净短波辐射通量和潜热通量 ,在季风爆发前后不同阶段 ,二个分量的变化有不同表现形式 ,但不论二者如何变化 ,季风爆发与活跃期 ,海面热收入减小或为净支出 ;季风爆发前及中断期间 ,海面热收入逐渐增加 ;由于大的热惯性 ,海温变化落后于海面热收支的变化 ,海温的这种滞后效应通过影响潜热通量调节海面热收支的变化 ,又反过来影响自身的变化 ,形成短期振荡过程 ,这种振荡过程与季风的活跃、中断过程相对应。 相似文献
653.
Large Aperture Scintillometer Used Over A Homogeneous Irrigated Area, Partly Affected By Regional Advection 总被引:3,自引:0,他引:3
Scintillometer measurements were collected over an irrigated wheat field ina semi-arid region in northwest Mexico. Conditions were unstable in the morning andstable during the afternoon, while latent heat fluxes remained high throughout the day.Regional advection was observed during near-neutral conditions. Monin–Obukhovsimilarity relationships for the structure parameter of temperature were verified in both unstable and stable conditions, but were violated close to near-neutral conditions. We found that, using additional measurements of radiation, soil heat flux and windspeed, areally averages of both sensible and latent heat fluxes can be reliably predicted by large aperture scintillometer measurements, as long as the net radiation is greater than zero. 相似文献
654.
南海深水区晚更新世以来沉积速率、沉积通量与物质组成 总被引:6,自引:2,他引:6
通过调查所获得柱样沉积物氧碳同位素测年资料及多学科综合分析表明,晚更新世以来南海沉积速率和沉积通量具有以下几个特征 :(1)总体上为间冰期沉积速率低、冰期沉积速率高,冰期沉积速率是间冰期沉积速率的 1.3~ 1.6倍;(2 )南海沉积速率趋势面分析表明,氧同位素 1期东北陆坡和西南陆坡沉积速率高,氧同位素 2、3期沉积速率分布特征相似,与 1期有所不同,东北陆坡沉积速率高于西南陆坡,表明氧同位素 2期之后,南海的沉积环境发生明显的改变,造成上述沉积速率分布的主要控制因素是南海周围的河流分布、季风、海流等;(3)南海东部沉积通量与物质组成分析表明,末次冰期以来沉积总通量北部陆坡区明显高于深海区,前者是后者 2~ 3倍,并有自北向南逐渐降低的趋势;(4)硅质生物沉积通量冰期明显高于间冰期,末次冰期以来东北部陆坡区的硅质生物沉积通量最高,末次冰期之前恰好相反,深海盆高于陆坡区;(5 )末次冰期以来,陆源沉积约占南海东部海域沉积的 4 4 %以上。 相似文献
655.
在2001年秋季对贵州省荔波县茂兰国家喀斯特森林公园林地、草地植被下土壤CO2呼吸释放及岩溶表层泉水HCO3及其δ13C值的变化进行了日动态的野外监测,表明岩溶系统中土-气-水界面间存在着碳交换的日动态变化以及所伴随的同位素交换的变化,这种变化与土温的日动态有密切的关系。林地植被显示了平抑这种日动态幅度的效应,而草地植被则显示响应于温度变化的较灵敏的动态变化。这种短尺度的变化构成了表层岩溶系统对外界条件的灵敏响应,进一步揭示了在生物作用下岩溶地质作用在碳循环过程及其同位素交换上的灵敏性和动态性。其不同植被系统下的日动态差异在解释岩溶沉积记录和讨论岩溶作用与碳循环时值得充分注意 相似文献
656.
1 INTRODUCTION AND REVIEW Numerous investigations related to vertical velocity and suspension concentration distributions have been undertaken to the steady, uniform, open channel turbulent flow. The problems of sediment mixed water flows are of direct interest to the practical situations in the field of river sedimentation, coastalsediment transport and in the field of two-phase flow in particular. In hydraulic open channel flow, the vertical velocity profile is usually described by… 相似文献
657.
Gottfried Hänel 《Pure and Applied Geophysics》1977,115(4):775-797
The dependency on relative humidity of the settling velocity of aerosol particles in stagnant air and of the diffusion coefficient due to Brownian motion of aerosol particles was computed for six aerosol types and different particles sizes in dry state. The computations are based (1) on mean bulk densities of dry aerosol particles obtained from measurements or from the knowledge of the chemical composition of the particles, (2) on micro-balance measurements of the water uptake per unit mass of dry aerosol substance versus water activity at thermodynamic equilibrium, and (3) on measurements of the equilibrium water activity of aqueous sea salt solutions. The results show a significant dependence of the settling velocity and Brownian diffusion of aerosol particles on relative humidity and on the particle's chemical composition.Nomenclature
A
surface parameter of a particle
-
B
surface parameter of a particle
-
c
L
velocity of sound in moist air
-
C
1+Kn[A+Qexp(–B/Kn]=slip correction
-
D
diffusion coefficient of a particle
-
D
1
D(=1)=diffusion coefficient of a spherical particle
-
f
P
w
/P
we
(T,P)=relative humidity (f=0 dry air,f=1 saturated air)
- g
acceleration due to gravity
-
g
|g|
-
k
1.3804×10–16 erg/°K=Boltzmann constant
-
Kn
L
/r=Knudsen number of a particle
-
Kn
0
0L
/r
0=Knudsen number of a dry particle
-
m
4r
3/3=mass of a particle
-
m
L
4r
3
L
/3=mass of the moist air displaced by a particle
-
M
mobility of a particle
-
M
0
molar mass of dry air
-
M
w
molar mass of water
-
Ma
|u–u
L
|/c
L
=Mach number of the particles motion relative to the ambient air
-
n
particle number per unit volume of air
-
P
P
0+P
w
=pressure of the moist air
-
P
0
partial pressure of the dry air
-
P
w
partial pressure of the water vapour
-
P
we
P
we
(T,P)=equilibrium partial water vapour pressure over a plane surface of water saturated with air
-
Q
surface parameter of a particle
-
r
equivalent radius of a particle (radius of a sphere with the particles volume)
-
r
0
equivalent radius of a particle in dry state
-
R
1+0.13Re
0.85=inertia correction
-
R
0
specific gas constant of dry air
-
R
w
specific gas constant of water
-
Re
2r
L
u–u
L
/
L
=Reynolds number of the particles motion relative to the ambient air
-
t
time
-
T
absolute temperature
- u
velocity of a particle
-
u
(amount of the) settling velocity of a particle in stagnant air
-
u
1
u(=1)=(amount of the) settling velocity of a spherical particle in stagnant air
- u
L
velocity of the ambient moist air (far enough from the particle where the flow pattern remains undistorted)
-
W
drag coefficient of a particles equivalent sphere
-
empirical parameter in equation (3.1)
-
dynamic viscosity of a particles liquid cover
-
L
dynamic viscosity of moist air
- 0L
dynamic viscosity of dry air (at the same pressure and temperature like the moist air)
-
celsius temperature
-
dynamic shape factor of a particle (=1 for a sphere)
- 0
dynamic shape factor of a dry particle
-
L
mean free path of the molecules in moist air
- 0L
mean free path of the molecules in dry air (at the same pressure and temperature like the moist air)
-
Po
mean free path of the molecules in dry air at the pressureP
0 of the dry air and the temperature given
-
factor of solid to liquid change-over (=1 for a solid particle)
-
mean bulk density of a particle
-
L
density of the moist air
- 0L
density of the dry air at the same pressure and temperature like the moist air
- 0
mean bulk density of a dry particle
- 0
mean diameter of the molecules of dry air
-
w
diameter of water molecules
-
relaxation time of a particle
-
gradient operation
-
3.141593 相似文献
658.
Settling velocities and entrainment thresholds of biogenic sands (shell fragments) under unidirectional flow 总被引:3,自引:0,他引:3
Settling velocities and entrainment thresholds of biogenic sedimentary particles, under unidirectional flow conditions, are derived on the basis of settling tower and laboratory flume experiments. Material consisting predominantly of equant blocks (shell fragments of Cerastoderma edule , density, ρ s =2800 kg m−3 ) or of mica-like flakes and elongate rods ( Mytilus edulis fragments, ρ s =2720 kg m−3 ) are used in separate series of experiments. Differences in the measured settling and threshold properties are related primarily to particle shape. The selection of a characteristic length scale for non-spherical grains is investigated by comparing two approaches used to define the grain size ( D ) of the sediment samples: grain settling and sieve analysis that are used to derive data for the threshold criteria, in terms of the Shields and Movability diagrams. The empirical curves effectively predict the threshold conditions for any grain shape, provided that grain size is defined in terms of grain settling velocity. However, a functional distinction is made between the characteristic `hydraulic' grain size, defined by grain settling for grain transport applications, and the actual (physical) grain size defined by sieve analysis. 相似文献
659.
青藏高原积雪异常对高原地面加热的影响 总被引:7,自引:0,他引:7
On the basis of snow data and AWS (Automatic Weather Station) data obtained from the Tibetan Plateau in recent years (1993 to 1999), the features of sensible heat, latent heat and net long-wave radiations are estimated, and their variations in more-snow year (1997/1998) and less-snow year (1996/1997) are analyzed comparatively. The relationships between snow cover of the Tibetan Plateau and plateau's surface heating to the atmospheric heating are also discussed. The difference between more-snow and less-snow year in spring is remarkably larger than that in winter. Therefore, the effect of anomalous snow cover of the Tibetan Plateau in winter on the plateau heating appears more clearly in the following spring of anomalous snow cover. 相似文献
660.
M. L. Wesely D. L. Sisterson R. L. Hart D. L. Drapcho I. Y. Lee 《Journal of Atmospheric Chemistry》1989,9(4):447-463
Eddy correlation measurements of NO vertical flux were made periodically from October 1983 through June 1984 at a height of eight meters above grass in northeastern Illinois, U.S.A. From 207 data points, each representing a 25 min average, 19 daytime cases and 8 nighttime cases were selected on the basis of steady, nonadvective atmospheric conditions. Each case was represented by a set of data constituting a 3 to 5 hr average. Concentrations of O3, NO, and NO
y
(from which NO2 was inferred) and local atmospheric and surface conditions also were measured, to provide the information necessary to assess the relative importance of surface deposition, surface emission, and air chemistry on the observed NO flux. On the basis of a linear regression analysis applied with independent variables representing physical, chemical, and biological processes, surface uptake of NO was very small for data primarily collected in the daytime during spring, and measured deposition velocities at a height of 8 m were very small, much smaller than expected for NO2. For the same time period, the surface emission rates of elemental nitrogen in NO were in the range of 1.4 to 4.2 ng m-2 s-1 for moist, unsaturated soils at temperatures near 15° C. These emissions were partially masked in the measured fluxes by rapid in-air chemical reactions involving O3 and NO2. The effects of rapid in-air chemical reactions involving O3 were to decrease the (upward) flux of NO with height. While the information collected at night was too limited to strongly support hypotheses concerning emissions and deposition, a pathway for NO production by reactions involving NO3 and related compounds was indicated. For daytime conditions, this production pathway is not evident, probably because of the relatively strong effects of photochemical reactions involving NO, NO2, and O3.Formerly with the Chemical Technology Division of Argonne National Laboratory and currently affiliated with Bio-Rad Laboratories, Digilab Division, Minneapolis, MN, U.S.A. 相似文献