全文获取类型
收费全文 | 7806篇 |
免费 | 1884篇 |
国内免费 | 2941篇 |
专业分类
测绘学 | 528篇 |
大气科学 | 4114篇 |
地球物理 | 1580篇 |
地质学 | 2912篇 |
海洋学 | 1566篇 |
天文学 | 87篇 |
综合类 | 622篇 |
自然地理 | 1222篇 |
出版年
2024年 | 57篇 |
2023年 | 165篇 |
2022年 | 329篇 |
2021年 | 389篇 |
2020年 | 423篇 |
2019年 | 506篇 |
2018年 | 417篇 |
2017年 | 428篇 |
2016年 | 452篇 |
2015年 | 506篇 |
2014年 | 625篇 |
2013年 | 685篇 |
2012年 | 688篇 |
2011年 | 666篇 |
2010年 | 487篇 |
2009年 | 612篇 |
2008年 | 509篇 |
2007年 | 658篇 |
2006年 | 509篇 |
2005年 | 501篇 |
2004年 | 407篇 |
2003年 | 331篇 |
2002年 | 271篇 |
2001年 | 258篇 |
2000年 | 244篇 |
1999年 | 224篇 |
1998年 | 224篇 |
1997年 | 169篇 |
1996年 | 142篇 |
1995年 | 148篇 |
1994年 | 127篇 |
1993年 | 117篇 |
1992年 | 78篇 |
1991年 | 54篇 |
1990年 | 51篇 |
1989年 | 41篇 |
1988年 | 38篇 |
1987年 | 18篇 |
1986年 | 10篇 |
1985年 | 17篇 |
1984年 | 11篇 |
1983年 | 7篇 |
1982年 | 11篇 |
1981年 | 7篇 |
1980年 | 5篇 |
1979年 | 1篇 |
1978年 | 3篇 |
1977年 | 2篇 |
1976年 | 1篇 |
1954年 | 2篇 |
排序方式: 共有10000条查询结果,搜索用时 62 毫秒
631.
江苏能源供应的严峻形势促使了地热资源的勘查和开发力度的加大;地热工作的实践和科学技术的进步,逐步扩大了其工作领域;浅层地温作为江苏地热资源开发利用的新领域被提上日程,依据现有资料,认为其前景广阔。 相似文献
632.
论"单位涌水量就是导水系数" 总被引:2,自引:0,他引:2
单位涌水量是井抽水水位降深换算为1 m时的单井出水量;导水系数是含水层宽度为1 m时,地下水水力坡度为1时的单宽流量.二者之间从定义上看毫无关系,但它们的单位(m3/d·m)(m2/d)是相同的.笔者经过多年探讨和初步试验后发现,单位涌水量就是管井抽水所利用含水层的导水系数. 相似文献
633.
Link between convection and meridional gradient of sea surface temperature in the Bay of Bengal 总被引:2,自引:0,他引:2
We use daily satellite estimates of sea surface temperature (SST) and rainfall during 1998–2005 to show that onset of convection
over the central Bay of Bengal (88–92°E, 14–18°N) during the core summer monsoon (mid-May to September) is linked to the meridional
gradient of SST in the bay. The SST gradient was computed between two boxes in the northern (88–92°E, 18–22°N) and southern
(82–88°E, 4–8°N) bay; the latter is the area of the cold tongue in the bay linked to the Summer Monsoon Current. Convection
over central bay followed the SST difference between the northern and southern bay (ΔT) exceeding 0.75°C in 28 cases. There was no instance of ΔT exceeding this threshold without a burst in convection. There were, however, five instances of convection occurring without
this SST gradient. Long rainfall events (events lasting more than a week) were associated with an SST event (ΔT ≥ 0.75°C); rainfall events tended to be short when not associated with an SST event. The SST gradient was important for the
onset of convection, but not for its persistence: convection often persisted for several days even after the SST gradient
weakened. The lag between ΔT exceeding 0.75°C and the onset of convection was 0–18 days, but the lag histogram peaked at one week. In 75% of the 28 cases,
convection occurred within a week of ΔT exceeding the threshold of 0.75°C. The northern bay SST, T
N
, contributed more to ΔT, but it was a weaker criterion for convection than the SST gradient. A sensitivity analysis showed that the corresponding
threshold for T
N
was 29°C. We hypothesise that the excess heating (∼1°C above the threshold for deep convection) required in the northern
bay to trigger convection is because this excess in SST is what is required to establish the critical SST gradient. 相似文献
634.
2-D Crustal thermal structure along Thuadara-Sindad DSS profile across Narmada-Son lineament,central India 总被引:1,自引:0,他引:1
Central India is traversed by a WSW-ENE trending Narmada-Son lineament (NSL) which is characterized by the presence of numerous
hot springs, feeder dykes for Deccan Traps and seismicity all along its length. It is divided in two parts by the Barwani-Sukta
Fault (BSF). To the west of this fault a graben exists, whereas to the east the basement is uplifted between Narmada North
Fault (NNF) and Narmada South Fault (NSF). The present work deals with the 2-D thermal modeling to delineate the crustal thermal
structure of the western part of NSL region along the Thuadara-Sindad Deep Seismic Sounding (DSS) profile which runs almost
in the N-S direction across the NSL. Numerical results of the model reveal that the conductive surface heat flow value in
the region under consideration varies between 45 and 47mW/m2. Out of which 23mW/m2 is the contribution from the mantle heat flow and the remaining from within the crust. The Curie depth is found to vary between
46 and 47 km and is in close agreement with the earlier reported Curie depth estimated from the analysis of MAGSAT data. The
Moho temperature varies between 470 and 500°C. This study suggests that this western part of central Indian region is characterized
by low mantle heat flow which in turn makes the lower crust brittle and amenable to the occurrence of deep focused earthquakes
such as Satpura (1938) earthquake. 相似文献
635.
渗漏是严重影响堤坝安全的主要形式,确定渗漏通道的位置是进行堤坝渗漏整治的前提和基础。温度场探测堤坝渗漏的研究是其中一种较便捷的方法,但是在理论上还需要进一步完善。在库水和地下水存在着温度差异的基础上,考虑堤坝发生集中渗漏后,渗漏通道中的地下水与周围土体进行热量交换,造成渗流通道附近地层温度发生改变,建立起温度场对渗漏通道的反演模型。在前人研究的基础上,考虑地温梯度的影响,可以建立有集中渗漏通道影响下的二维热传导方程,进而以现场测井的温度数据作为边界条件,对泛定方程进行求解,最终得到渗漏通道的位置。计算结果和实测结果的对比表明,通过温度场反推渗漏通道参数的方法是可行的。 相似文献
636.
通过对不同温度、盐分和干旱胁迫对刚毛柽柳种子萌发实验研究影响,结果表明:刚毛柽柳种子的适宜萌发温度范围为10~35℃,萌发率高达80%以上,且萌发迅速。不同浓度NaCl溶液对刚毛柽柳种子萌发有明显抑制作用,种子萌发率随NaCl溶液浓度的增大而下降,到0.7 mol/L时,萌发率仅为1.67%,种子发芽受到抑制。相同渗透势PEG-6 000溶液中的萌发率低于NaCl溶液,渗透势为-0.5 MPa是二者影响作用的分界点。渗透势为-1.8 MPa时,萌发率已急剧下降到0,其对种子萌发的抑制作用大于NaCl溶液。将在两溶液中处理10天的种子转移至蒸馏水后,随着NaCl溶液浓度的增大,萌发恢复率逐渐升高,0.7 mol/L时,萌发恢复率为60%;随着PEG-6 000溶液浓度增大,萌发恢复率先升高后降低,渗透势为-1.4 MPa时,种子萌发恢复率达到最大为67.5%,但两种处理下种子的最终萌发率(总萌发率)都低于在蒸馏水中的。 相似文献
637.
隆冬异常升温北疆积雪提前融化 总被引:1,自引:0,他引:1
2007年1月下旬中期开始,新疆北部地区出现了一次异常的升温天气过程,1月27日~2月4日的9d中,北疆各地的43个气象站中,有14站的日最高气温突破同期历史极值,其中伊犁河谷的新源的日最高气温上升到13.3℃,突破同期历史极值3.0℃;有19站的9天平均气温突破同期历史极值,占总站数的44.2%。1月下旬本是新疆北部的积雪稳定积累期,但是2007年元月下旬异常升温天气的出现和持续,使北疆地区积雪提前融化,到2月初,北疆的博尔塔拉蒙古自治州、伊犁地区、乌鲁木齐市等地的积雪面积明显减少,乌鲁木齐地区的积雪覆盖度仅为25.84%,比15年同期平均值偏少5成。冬季是新疆增温幅度最大的季节,在气候变暖背景下,冬季极端天气气候事件的出现也越来越频繁,隆冬季节的异常升温造成气温偏高,使北疆地区的积雪提前融化。这些变化将对新疆水资源的时空分布产生重大影响,对当地生态环境将带来难以估测的影响。在全球气候变化背景下,更加需要加强对新疆等干旱地区极端天气气候事件的监测分析及其对生态环境、经济社会发展的影响等诸多领域的研究,使社会各界以积极的态度来科学客观地认识气候变化带来的后果,及早提出应对区域气候变化的对策,采取切实可行的措施减缓气候变化带来的负面影响。 相似文献
638.
利用天气数值预报产品建立贵州黔西南州分县温度预报方程的方法及应用 总被引:1,自引:0,他引:1
利用2002~2004年1~12月EC、T213天气数值产品的温度格点实时分析资料、预报资料以及贵州省黔西南州8个测站观测资料,从160个样本中筛选出相关较好的因子,利用多元回归统计模型,以及根据地理环境,天气形势分型造成的温度差值(ΔT)为逐步订正值,建立黔西南州分县温度预报方程。在2005年11月~2006年2月应用中取得较好效果,预报误差小于±3.0℃,平均误差1.3℃。 相似文献
639.
Paula Arcari Nigel Tapper Sharron Pfueller 《Singapore journal of tropical geography》2007,28(3):251-272
Since 1970, the worldwide distribution, frequency and intensity of epidemics of dengue and dengue haemorrhagic fever (DHF) have increased dramatically. In Indonesia, as elsewhere, the geographic distribution and behaviour of the two main vectors – Aedes aegypti and Aedes albopictus – and the consequent transmission dynamics of the disease are strongly influenced by climate. Monthly incidence data were examined in relation to monthly data for temperature, rainfall, rainfall anomalies, humidity and the Southern Oscillation Index for 1992–2001. Focusing on eight provinces, significant Pearson correlations were observed between dengue/DHF incidence and at least one climate variable ( r = ±0.2 to ±0.43; P < 0.05). Multiple regression analyses showed that 12.9–24.5 per cent of variance in incidence was explained by two or three climate variables in each province ( P < 0.1–0.01). Rainfall appears to be the principal climatic agent affecting the geographic distribution and temporal pattern of incidence while temperature appears to play a critical role in outbreak intensity. Wide regional and temporal variations in the strength and nature of the observed associations led to the identification of three groups of provinces where increases in dengue/DHF incidence were variously associated with increased rainfall, decreased rainfall and/or high susceptibility to climate variability. Although climatic factors play an important role in explaining the timing and intensity of dengue/DHF outbreaks, a wide range of other factors specific to local environments also appear to be involved – information that may assist in the prediction and mitigation of regional dengue/DHF outbreaks. 相似文献
640.
Three-dimensional thermal structure of the Chinese continental crust and upper mantle 总被引:3,自引:0,他引:3
We invert S-wave velocities for the 3D upper-mantle temperatures, in which the position with a temperature crossing the 1300℃ adiabat is corresponding to the top of the seismic low velocity zone. The temperatures down to the depth of 80 km are then calculated by solving steady-state thermal conduction equation with the constraints of the inverted upper-mantle temperatures and the surface temperatures, and then surface heat flows are calculated from the crustal temperatures. The misfit between the calculated and observed surface heat flow is smaller than 20% for most regions. The result shows that, at a depth of 25 km, the crustal temperature of eastern China (500―600℃) is higher than that of western China (<500℃). At a depth of 100 km, temperatures beneath eastern and southeastern China are higher than the adiabatic temperature of 1300℃, while that beneath west China is lower. The Tarim craton and the Sichuan basin show generally low temperature. At a depth of 150 km, temperatures beneath south China, eastern Yangtze craton, North China craton and around the Qiangtang terrane are higher than the adiabatic temperature of 1300℃, but is the lowest beneath the Sichuan basin and the regions near the Indian-Eurasian collision zone. At a depth of 200 km, very low temperature occurs beneath the Qinghai-Tibet Plateau and the south to the Tarim craton. 相似文献