全文获取类型
收费全文 | 8122篇 |
免费 | 1116篇 |
国内免费 | 1006篇 |
专业分类
测绘学 | 587篇 |
大气科学 | 1254篇 |
地球物理 | 2628篇 |
地质学 | 3572篇 |
海洋学 | 584篇 |
天文学 | 450篇 |
综合类 | 526篇 |
自然地理 | 643篇 |
出版年
2024年 | 13篇 |
2023年 | 37篇 |
2022年 | 146篇 |
2021年 | 202篇 |
2020年 | 142篇 |
2019年 | 151篇 |
2018年 | 594篇 |
2017年 | 543篇 |
2016年 | 424篇 |
2015年 | 302篇 |
2014年 | 308篇 |
2013年 | 312篇 |
2012年 | 872篇 |
2011年 | 620篇 |
2010年 | 304篇 |
2009年 | 308篇 |
2008年 | 270篇 |
2007年 | 280篇 |
2006年 | 249篇 |
2005年 | 960篇 |
2004年 | 975篇 |
2003年 | 728篇 |
2002年 | 260篇 |
2001年 | 161篇 |
2000年 | 142篇 |
1999年 | 115篇 |
1998年 | 125篇 |
1997年 | 124篇 |
1996年 | 85篇 |
1995年 | 71篇 |
1994年 | 77篇 |
1993年 | 57篇 |
1992年 | 50篇 |
1991年 | 49篇 |
1990年 | 37篇 |
1989年 | 28篇 |
1988年 | 23篇 |
1987年 | 19篇 |
1986年 | 15篇 |
1985年 | 3篇 |
1984年 | 5篇 |
1983年 | 5篇 |
1982年 | 4篇 |
1980年 | 6篇 |
1976年 | 3篇 |
1975年 | 4篇 |
1965年 | 3篇 |
1954年 | 2篇 |
1951年 | 2篇 |
1948年 | 2篇 |
排序方式: 共有10000条查询结果,搜索用时 31 毫秒
41.
钝顶螺旋藻部分原生质体及单细胞的制备与培养 总被引:21,自引:0,他引:21
于1992年1月-1994年4月,进行超声波处理方法制备钝顶螺旋藻部分原生质体以作为基因工程受体,以及制备单细胞用于固体平板克隆化培养的研究。研究结果表明:超声波以20kHz频率、15W功率作用30s,可使藻丝体断裂成15.0±1.6个细胞长度;延长作用时间,至2-6个细胞长度时,细胞壁结构遭到破坏,形成部分原生质体;继续作用,可形成少量原生质体和大量单细胞。断裂藻丝体、部分原生质体、单细胞以及原生质体均可涂布于固体培养基上再生或生长。以一定密度涂布单细胞与原生质体,能够形成彼此分开的单个克隆,可用于筛选及遗传分析。本文提供了一种节省溶菌酶的制备螺旋藻透性体的方法,超声波作用利于外源基因的导入,而涂布培养利于进一步的筛选和形成克隆。 相似文献
42.
秦曾灏 《中国海洋大学学报(自然科学版)》1987,(3)
本文着重研究大地形对正压大气迭加在非均匀纬向基本气流上挑动演变的影响。用WKBJ方法推导了正压扰动的频率和频散关系以及波作用量所满足的方程。当基本流场定常且存在无限长的东西向山脉时,则有波作用量守恒。据此,获得了正压不稳定的必要条件:即在所考察的平面域内至少在某点或某些点上含地形效应的某一物理量等于零,扰动就可能得到发展。对波包动能的倚时变化的讨论得知,在无摩擦正压纬向非均匀基流的情形,地形对扰动动能并无直接影响,即导波和曳波分别在西风急流的南侧和北侧得到加强,并分别在西风急流的北侧和南侧强度减弱。扰动的发展由扰动的结构所决定。导波和曳波的波长缩短总伴同其轴线倾向于东西向相联系,而它们的波长伸长总是与其轴线倾向于南北向同时发生。还指出,正压扰动的加强(或减弱)与波长的伸长(或缩短)不是必然的联系,它的成立是有条件的。 相似文献
43.
44.
45.
Size-Fractionated Primary Production Estimated by a Two-Phytoplankton Community Model Applicable to Ocean Color Remote Sensing 总被引:3,自引:0,他引:3
In order to estimate primary production from ocean color satellite data using the Vertical Generalized Production Model (VGPM; Behrenfeld and Falkowski, 1997), we propose a two-phytoplankton community model. This model is based on the two assumptions that changes in chlorophyll concentration result from changes of large-sized phytoplankton abundance, and chlorophyll specific productivity of phytoplankton tends to be inversely proportional to phytoplankton size. Based on the analysis of primary production data, P
opt
B
, which was one parameter in the VGPM, was modeled as a function of sea surface temperature and sea surface chlorophyll concentration. The two-phytoplankton community model incorporated into the VGPM gave good estimates in a relatively high productive area. Size-fractionated primary production was estimated by the two-phytoplankton community model, and P
opt
B
of small-sized phytoplankton was 4.5 times that of large-sized phytoplankton. This result fell into the ranges observed during field studies. 相似文献
46.
-Mainly on the basis of the data obtained during PRC/US bilateral TOGA cruises, abnormal variation occurred during the 1986/1987 El Nino is shown in this paper about the thermal structure and circulation of the upper western tropical Pacific Ocean. The effects of the abmormal variation on the subtropical high over the Northwest Pacific Ocean are discussed. During the El Nino: (1) In the east part of the western tropical Pacific Ocean (the subsurface temperature data on the 165° E section are taken as an example), the water wanner than 29 C in the upper layer spread on the longitudinal section and positive temperature anormalies appeared in a large area of the sea surface. (2) In the west part of the western tropical Pacific Ocean (the subsurface temperature data on the 137°E section are representative ), the cross section occupied by the upper layer warmer water ( T >28 ℃ ) became shrunk, and the sea surface temperature showed negative amomalies. (3) The eastward flows in the upper layer of the 165° 相似文献
47.
Long-term Sensor Drift Found in Recovered Argo Profiling Floats 总被引:5,自引:0,他引:5
We recovered three Argo profiling floats after 2 to 2.5 years of operation, and recalibrated their temperature, conductivity, and pressure sensors. The results demonstrate that these floats exhibited a significant drift in salinity of −0.0074 to −0.0125, primarily due to the conductivity sensor drift. Combined with the recalibration result for another previously recovered float, the indication is that the negative salinity drift increases nearly in proportion to the operating period of floats. The increasing rate is −0.0041 (±0.0015) year−1, which yields a salinity drift of −0.016 (±0.006) for the expected float lifetime of four years. The present result suggests that reducing the float surfacing time would improve the accuracy of the salinity measurements. 相似文献
48.
Takushi?NikiEmail author Taiki?Fujinaga Mariyo?F.?Watanabe Junji?Kinoshita 《Journal of Oceanography》2004,60(5):913-917
Solid-phase microextraction (SPME) is a simple, sensitive and less destructive method for the determination of dimethylsulfide
(DMS) in seawater. Combined with detection by gas chromatography-mass spectrometry (GC-MS), the method had sufficient sensitivity
(minimum detectable concentration of DMS was 0.05 nM), and practical levels of reproducibility (relative standard deviation
≤7%) and linearity (r
2 > 0.995) over a wide concentration range (0.5 to 910 nM). The protocol developed was applied to a Sagami Bay water sample
to determine concentrations of DMS and DMSP, and in situ DMSP-lyase activity. 相似文献
49.
Eddy Shedding from the Kuroshio Bend at Luzon Strait 总被引:16,自引:1,他引:16
TOPEX/POSEDIENT-ERS satellite altimeter data along with the mean state from the Parallel Ocean Climate Model result have been used to investigate the variation of Kuroshio intrusion and eddy shedding at Luzon Strait during 1992–2001. The Kuroshio penetrates into the South China Sea and forms a bend. The Kuroshio bend varies with time, periodically shedding anticyclonic eddies. Criteria of eddy shedding are identified: 1) When the shedding event occurs, there are usually two centers of high Sea Surface Height (SSH) together with negative geostrophic vorticity in the Kuroshio Bend (KB) area. 2) Between the two centers of high SSH there usually exists positive geostrophic vorticity. These criteria have been used to determine the eddy shedding times and locations. The most frequent eddy shedding intervals are 70, 80 and 90 days. In both the winter and summer monsoon period, the most frequent locations are 119.5°E and 120°E, which means that the seasonal variation of eddy shedding location is unclear. 相似文献
50.