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实测和回归分析鄱阳湖鲌属(Culter)的翘嘴鲌(C.alburnus)、蒙古鲌(C. mongolicus)、达氏鲌(C.dabryi)和原鲌属(Culterichthys)的红鳍原鲌(C. erythropterus)体重与体维关系.结果表明,多元回归方程能全面地反映不同体维对鱼类体重的影响,体重与体侧面积体厚的回归方程较适宜.其体重(W)与体侧面积(A)及体厚(T)的幂函数关系式分别是,翘嘴鲌:W=4.05051×10-3A0.66260T1.41994;蒙古鲌:W=3.18603×10-3A0.66845 T1.44376;达氏鲌:W=1.99310×10-3A0.70982T1.47305;红鳍原鲌:W=3.58823×10-3A0.63253T1.49465. 相似文献
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香蒲、灯心草人工湿地的研究─Ⅱ.净化污水的空间 总被引：26，自引：0，他引：26
应用测定流水中溶氧量的方法,测定了长薄鳅的耗氧率,耗氧量及窒息点．试验表明：长薄鳅的耗氧率（Ｙ’）随鱼体重（Ｗ,ｇ）的增加而增大,其关系式分别为：Ｙ’＝１８６．５７６Ｗ（－０．２０４３）,Ｙ＝０．１８６Ｗ（０．７９６２）．温度对长薄鳅的耗氧率有影响,在１３－３０Ｃ范围内,耗氧率随水温升高而逐渐增大．耗氧率的温度敏感区域是１３－２３Ｃ和２８－３０Ｃ,而在２３－２８Ｃ范围内变化幅度较小,标准代谢量变化 相似文献
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共和盆地位于青藏高原东北缘，是我国重要的干热岩地热资源赋存区之一．成因机制研究是干热岩地热资源研究中最为基础与核心的工作之一，也是干热岩地热资源潜力精细评价和合理开发利用的重要依据．本文基于98块采自共和—贵德盆地岩石样品的放射性生热率数据，分析了盆地主要岩性岩石的放射性生热率分布特征，讨论了共和盆地干热岩地热资源的成因机制，并初步建立了干热岩地热资源的成因模式．研究表明，共和盆地恰卜恰地热区沉积岩（以泥岩和粉砂质泥岩为主）放射性生热率为1.21～2.02μW·m~(-3)，平均值为1.67±0.29μW·m~(-3)；以花岗岩和花岗岩闪长岩等为主的基底岩石的放射性生热率介于1.17～5.81μW·m~(-3)之间，平均值为3.20±1.07μW·m~(-3)．贵德盆地扎仓寺地热区沉积岩（以砂岩和泥质砂岩为主）放射性生热率为1.83～2.40μW·m~(-3)，平均值为2.13±0.23μW·m~(-3)；基底花岗质岩石的放射性生热率介于0.92～6.49μW·m~(-3)之间，平均值为2.81±1.40μW·m~(-3)．测试数据显示共和—贵德盆地基底花岗岩不存在高放射性生热率异常．但是，新生代以来印度—欧亚板块持续性陆-陆碰撞作用造成的壳内放射性生热元素富集层增厚，导致了花岗岩放射性生热率的热贡献量同步增大（30.3～40.5mW·m~(-2)），因此，花岗岩放射性生热可为共和盆地干热岩地热资源提供稳定的壳内热源基础．基于放射性生热率数据和热流配分研究，结合研究区已有地质-地球物理研究资料，本文认为壳内部分熔融层作为附加热源为共和盆地干热岩地热资源提供了重要的附加热流贡献．在此基础上，本文初步构建了共和盆地干热岩地热资源成因模式：加厚地壳花岗岩放射性生热与壳内部分熔融层供热． 相似文献
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依据中国大陆科学钻探(CCSD)两口先导孔中地热测量和岩石样品热物性参数,对5000m深钻的可能钻遇温度进行了预测.先导孔中地温梯度介于1-26℃/km;岩石热导率变化为2.64-8.81W/(m@K),平均(3.4±1.26)W/(m@K);实测热流值为76-80mW/m2;30块岩石样品放射性生热率变化为(0.0-2.17)μW/m3,450m深度以上层平均(0.76±0.5)μW/m3,以下层段平均(0.48±0.2)μW/m3,生热率随深度递减,但变化趋势难以明确判定.分别对热流和热导率取上、下限,采用不同的生热率随深度的分布函数,区分考虑或不考虑热导率的温度相关性,分别计算出5000m深度内可能的温度分布剖面.计算结果表明,超深井于5000m垂直深度上的温度将达到110-140℃,2000m深度的探井钻遇温度将介于54-64℃.此外,考虑热导率的温度效应后预测的温度一般高于未考虑热导率温度效应5-8℃. 相似文献
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比较分析了我国南亚热带湖库7种常见浮游动物,萼花臂尾轮虫(Brachionus calyciflorus)、前节晶囊轮虫(Asplanchna priodonta)、颈沟基合溞(Bosminopsis deitersi)、微型裸腹溞(Moina micrura)、中华拟同型溞(Daphnia similoides sinensis)、温中剑水蚤(Mesocyclops thermocyclopoides)和舌状叶镖水蚤(Phyllodiaptomus tunguidus)在温度15~30℃范围内的氮、磷排泄率以及氮、磷含量.氮、磷含量分别为4.9~24.2μg/mg(DW)和51.2~153.5μg/mg(DW);氮磷原子比为11.5~43.0.磷含量与个体干重呈显著正相关关系,但氮含量和氮磷比与个体干重相关性不显著.溶解态无机磷(DIP)排泄率为0.31~2.05μg/(mg(DW)·h),与个体干重呈显著负相关,与温度和个体氮磷含量比值均呈显著正相关.总溶解态氮(TDN)排泄率为24~256μg/(mg(DW)·h),与温度和个体干重均呈显著相关,但与个体氮磷含量比值相关性不显著.排泄的TDN∶DIP原子比为112~352,与温度呈显著正相关,与个体干重和氮磷含量比值均呈显著负相关.结果表明,在高氮磷比的食物条件下,7种浮游动物营养盐排泄均呈现高的氮磷比特征,磷排泄率和排泄的氮磷比的种间差异受个体干重和个体氮磷比影响. 相似文献
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2002-2004年，在浙江衢州铜山源水库，对该库放养的美国大口胭脂鱼的生长情况进行了研究，结果表明，该水 库美国大口胭脂鱼的鳞片以环片的切割型为主要年轮特征．用刺网所捕的美国大口胭脂鱼渔获物中以Ⅱ、Ⅲ、Ⅳ龄个体为 主．体长和体重的关系式为：W=8．595×10~(-5)15 L~(2.662)，Von Bertalanffy 生长方程的主要生物学参数：L_∞=36．54cm，W_∞= 1．245kg，K=0．6377，t_0=-0．261龄，体重生长的拐点年龄 t_1=1．92龄，拐点体重W_1=0．396kg．与池养鱼类生长情况相 比，铜山源水库的美国大口胭脂鱼生长较慢． 相似文献
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地幔主要矿物橄榄石［(Mg089Fe011)2SiO4］的相变与深源地震的解释以及俯冲带和周围地幔的相互作用相关. 其中，形核率和长大率是刻画其相变动力学的两个重要参数. 因为实验技术的原因，目前人们还没有基于实验数据给出橄榄石的形核率. 本文首先通过对挤碰物理图像的分析，对边界形核情形的相变动力学理论中表征挤碰程度的无量纲参数进行了修正. 在此基础上，根据已有的实验资料，首次对橄榄石相变的形核率进行了估计. 通过对形核率数据的拟合，可以得到形核率参数K0和γ1/3. 得到两个形核率参数的变化范围分别为K0=55×1021～87×1027s-1·m-2·K-1，γ1/3=0～020 J·m-2，最佳拟合值为：K0=69×1024s-1·m-2·K-1，γ1/3=016 J·m-2. 相似文献
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在不同温度下,对太湖河蚬进行了室内短期氮、磷释放模拟实验.结果表明,温度对河蚬(Corbicula fluminea)不同形态氮、磷的排泄都有重要的影响.总磷(TP)、总氮(TN)、总溶解性氮(TDN)、总溶解性磷(TDP)和正磷酸盐(PO3-4-P)排泄率随温度的升高都显著升高,而亚硝态氮(NO-2-N)排泄率先升高后下降.铵态氮(NH+4-N)排泄率在5和15℃间变化不显著,温度对硝态氮(NO-3-N)排泄率有影响但不显著.同时实验发现河蚬为排氨动物,NH+4-N排泄占TN排泄的50.78%~100%,TDN排泄占TN排泄的89.14%~100%,而NO-3-N、NO-2-N虽都有检出,但所占比例相对较小.在河蚬磷排泄中,TDP占TP比例范围为83.01%~100%,PO3-4-P在36.60%~96.59%之间,且所占比例都有随温度升高而增加的趋势.同时对排泄率与干重和温度之间的关系进行了回归分析,发现不同氮、磷排泄率(NO-3-N和NO-2-N除外)与温度和干重的关系均符合方程R(X)=a Wb·ec T+d,决定系数R2都在0.967以上. 相似文献
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珊瑚δ^18Oc,Sr／Ca和Mg／Ca比值是海水表面温度SST的指示剂,需要采用室内的珊瑚养殖实验给于验证．本文利用新型的室内珊瑚养殖水循环系统和新生长珊瑚培植方法,进行了不同海水温度孔21—28℃）下的鹿角珊瑚的养殖实验,对养殖珊瑚δ18Oc,Sr／Ca和Mg／Ca进行了测定．结果表明,养殖珊瑚δ18Oc,Sr／Ca和Mg／Ca与r均呈现出明显的相关性,线性回归曲线为δ18Oc（‰）=-0．1427×孔℃）-0．1495（n=18,r=-0．955,P〈0．0001）,斜率-0．1427％d℃落在文献发表值范围（-0．13—0．29％d℃）的低端,Sr／Ca比值随r的上升而下降．而对Mg／Ca比值则相反,随丁的升高而增加,Sr／Ca与Mg／Ca呈现负相关关系,其线性回归曲线分别为Sr／Ca（mmol／m01）=-O．04156×T＋10．59（n=15,r=-0．789,P〈0．005）,Mg／Ca（mmol／m01）=0．04974×T＋2．339（n=17,r=-0．457,P〈0．05）,表明Mg／Ca和Sr／Ca每增加1mmol／mol时,记录的丁分别升高5．19℃和降低15．62℃,这些数值均明显低于文献所发表值,文章对此进行了初步讨论． 相似文献
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For successful snowdrift modelling, measured drift shapes should be geometrically similar to full-scale shapes and develop at rates that scale in a known manner. Consensus exists on most modelling methods and the similitude requirements needed to meet these objectives. A notable exception is the manner to scale drift development rates. A rationale is presented for rate scaling based on an independent model and prototype mass transport measurements. This approach is validated by comparing the rate of drift development for a model Wyoming snow fence with corresponding field data. This method yields excellent agreement, whereas the alternatives differ substantially. 相似文献
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Wendy Freedman 《Astronomy& Geophysics》2002,43(1):1.10-1.13
Wendy Freedman presents the 2001 George Darwin Lecture on present and future advances in cosmology.
Modern cosmology is undergoing an explosion of observational and experimental results that is in turn driving significant theoretical advances and a dynamic interface between theory and experiment. As a consequence, cosmological parameters are becoming much more precisely constrained. In this, the George Darwin lecture for 2001, I look back at the some of the advances made since Edwin Hubble presented his George Darwin lecture in 1953, and look ahead to the resolution of significant cosmological uncertainties. 相似文献
Modern cosmology is undergoing an explosion of observational and experimental results that is in turn driving significant theoretical advances and a dynamic interface between theory and experiment. As a consequence, cosmological parameters are becoming much more precisely constrained. In this, the George Darwin lecture for 2001, I look back at the some of the advances made since Edwin Hubble presented his George Darwin lecture in 1953, and look ahead to the resolution of significant cosmological uncertainties. 相似文献
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Recent observations made by Kanamori and Allen about earthquake recurrence time and average stress drop revealed a very interesting relation: earthquakes with longer recurrence times have higher average stress drops. They attributed the difference in stress drop to the difference in long-term average slip rate. To interpret their result in terms of the healing effect, we simulated earthquake recurrence with a one-dimensional mass-spring model, incorporating a recently developed rate-and-state dependent friction law for different loading rates and heterogeneous strength distributions. We first calculated the stress drop and recurrence time as functions of loading rate for a homogenous fault model. We found that the stress drop increases up to 30% when the loading rate decreases from 10 cm/yr to 0.01 mm/yr. Thus, the observed great variability of stress drop, from a few bars to a few hundred bars, which is obtained by replotting the data of Kanamori and Allen in the form of stress drop versus long-term slip rate, may not be attributable to the healing effect alone. Our numerical simulation shows that the variability may be due primarily to the spatial heterogeneity of strength on the fault. Our simulation also suggests that of the two empirical laws that were inferred from the same laboratory friction data, called the power law and the logarithmic law by Shimamoto and Logan, the former can explain the observed relation between stress drop and slip rate better than can the latter, at least for strike-slip fault. The logarithmic law is an earlier and simpler version of the rate-state-dependent friction law. 相似文献
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Precipitation collected in continuously open containers for about a year at seven sites around the United States was analyzed for10Be,90Sr,210Pb and238U. Based on these data and long-term precipitation,90Sr and210Pb delivery patterns, the stratospheric, tropospheric and recycled10Be components in the collections were estimated and the global10Be production rate was assessed. Single station production rate estimates range from 0.52 × 106 atoms cm−2 yr−1 to 2.64 × 106 atoms cm−2 yr−1. The mean value is 1.21 × 106 atoms cm−2 yr−1 with a standard error of 0.26 × 106 atoms cm−2 yr−1. 相似文献
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《国际泥沙研究》2020,35(6):563-575
Erosion of mixed cohesive and noncohesive sediments is studied using the erosion test instrument SEDFlume. The sediment mixtures are composed of well-sorted quartz sand (0.25–0.5 mm) and one of the three used muds: kaolinite, kaolinite-bentonite and Mississippi River muds. The mud contents cover from 0 to 100%. The measured data of erosion rate and bed shear stress are used to examine the segmented linear, nonlinear, and exponential erosion models. The parameters of each erosion model are related to the physical properties of sediment mixtures, including clay fraction, mud fraction, mixture dry density, and mud dry density. It is found that the three models can fit well with the data, and their parameters have strong relations with the mud fraction and mud dry density, to a less extent with the clay fraction, but not with the mixture dry density. 相似文献
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Micheline C. Roufosse 《Physics of the Earth and Planetary Interiors》1979,19(4):348-354
Steady-state creep in the earth's mantle is controlled by the diffusion coefficient and by the distances traveled by defects between sources and sinks. In this paper, we investigate the role played by additional vacancies created by natural radioactivity. According to recent studies, bombardment of solids by energetic particles can act as a perturbation. The resulting strain rate is proportional to the rate of vacancy creation and, contrary to ordinary creep mechanisms, is only weakly dependent on the temperature and the energy necessary to create those vacancies; it is independent of the grain size. The strain rate is of the same order of magnitude as the diffusion mechanism but smaller than the dislocation-climb rate by two to three orders of magnitude. Consequently, the strain rate produced by natural radioactivity does not play a major role in the observed rate of deformation, although it could constitute a lower limit to the creep rate and act as a regulatory mechanism. Furthermore, being less strongly affected by temperature and the vacancy-formation energy than are the other mechanisms, it is also less strongly affected by depth. 相似文献
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由给定的随时间和空间变化的二维应变速率分布计算速度场,根据速度场计算二维热传导方程,得到岩石圈的热演化结构,然后计算由热扰动引起的密度变化,进而确定加载到岩石圈上的载荷,根据载荷计算挠曲方程,最终得到盆地的沉降.在此基础上讨论了热源对地表热流和沉降的影响以及岩石圈有效弹性厚度对盆地几何形态的影响.结果表明,热源对地表热流影响显著,对沉降影响不大,岩石圈有效弹性厚度则控制盆地的几何形态.二维应变速率正演为下一步的反演奠定了基础. 相似文献