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44.
影响海洋微藻生产麻痹性贝类毒素的重要生态因素 总被引:1,自引:0,他引:1
麻痹性贝类毒素是有害赤潮海洋微藻生产的重要毒素种类,本文综述了影响该类毒素的主要生态因素有光,温度,盐度和营养盐4类;弱光对毒素合成有抑制作用。低温下PSP毒素产量高,通过对营养盐吸收机制的离子效应,盐度可影响毒素的生命合成,不同种类和株系对N、P限制的反应有极大差异。 相似文献
45.
HL-1装置中LHCD和等离子体参数的关系 总被引:1,自引:1,他引:0
本文研究了在HL-1托卡马克的不同放电阶段的低混杂波驱动特性。给出了驱动电流及驱动效率和等离子体参数,如电子平均密度ne、等离子体电流Ip及纵向磁场的关系。也给出和分析了波驱动和入射波功率的关系。在放电平段,对正反向驱动效率进行了研究和比较。 相似文献
46.
微分脉冲溶出伏安法同时测定食品中的锌铁锰 总被引:7,自引:4,他引:3
在1%乙二胺-0.1mol/L酒石酸钠-pH11.82 Britton—Robinson缓冲溶液体系中用微分脉冲溶出伏安法同时测定锌、铁、锰三种微量元素。它们的峰电位分别为-1184,-1392和-1456mV(vs.Ag/AgCl);线性范围分别为:0.001—0.015,0.005—0.05和0.04—0.7μg/mL,最低检出浓度分别为0.0007,0.0014和0.0193μg/mL。本法操作简便、准确、灵敏度较高,用于食品中这三种元素的分析,结果令人满意。 相似文献
47.
On the Rank of the Semigroup TE(X) 总被引:1,自引:0,他引:1
Pei Huisheng 《Semigroup Forum》2005,70(1):107-117
${\cal T}_X $ denotes the full transformation semigroup on a set $ X $. For a
nontrivial equivalence $E$ on $X$, let
\[
T_E (X) =\{ f\in {\cal T}_X : \forall \, (a,b)\in E,\, (af,bf)\in E \} .
\]
Then $T_E (X) $ is exactly the semigroup of continuous selfmaps of
the topological space $X$ for which the collection of all
$E$-classes is a basis. In this paper, we first discuss the rank
of the homeomorphism group $G$, and then consider the rank of $T_E
(X)$ for a special case that the set $X$ is finite and that each
class of the equivalence $E$ has the same cardinality. Finally,
the rank of the closed selfmap semigroup $\Gamma(X)$ of the space
$X$ is observed. We conclude that the rank of $G$ is no more than
4, the rank of $T_E (X)$ is no more than 6 and the rank of
$\Gamma(X)$ is no more than 5. 相似文献
48.
Zhi‐Yong Huang Jin‐Can Shen Zhi‐Xia Zhuang Xiao‐Ru Wang Frank S. C. Lee 《应用有机金属化学》2004,18(6):255-261
Cinnabar, as one of the most widely used mineral drugs in traditional Chinese medicines, has been proven to have prominent curative effects in clinical use for more than 2000 years. But the safety and toxicity of the drug has been under constant debate in clinic usage. Metallothionein (MT) contains about 30% of cysteine in the molecule, and plays an important detoxification role against heavy metals. In this study, it was used as a biomarker to assess mercurial accumulation in rats fed orally with cinnabar. After feeding rats with cinnabar by gastric gavage at different dosages and at different times, the distribution of heavy metals (including mercury, copper and zinc) and MT was investigated among rat tissues, including liver, kidney, heart, brain, testis and blood. Metals and MT determinations were carried out using inductively coupled plasma mass spectrometry (ICP‐MS) and a modified mercury saturation assay technique respectively. The results indicated that mercury was easily accumulated in the tissues of rats exposed to cinnabar, especially in kidney. For example: at a feeding dosage of 5 g kg?1 (bw) for 4 weeks, the mercury concentrations in kidney were 13, 8.7, 21.6 and 26 times those in liver, testis, brain and heart respectively; and at 2.5 g kg?1 (bw) for 2 weeks, the mercury concentrations in kidney were 21, 2.1, 3 and 21 times those in liver, testis, brain and heart respectively. In addition, mercury in kidney and liver of all cinnabar groups was significantly higher than that of the control group (P < 0.01). A high positive correlation observed between MT concentrations and mercury levels in both liver and kidney (R2 = 0.9299, P < 0.02 for liver; R2 = 0.9923, P < 0.0008 for kidney) indicated that MT could be used as a biomarker for mercury in tissues. Copyright © 2004 John Wiley & Sons, Ltd. 相似文献
49.
In this paper, a projection method is presented for solving the flow problems in domains with moving boundaries. In order to track the movement of the domain boundaries, arbitrary‐Lagrangian–Eulerian (ALE) co‐ordinates are used. The unsteady incompressible Navier–Stokes equations on the ALE co‐ordinates are solved by using a projection method developed in this paper. This projection method is based on the Bell's Godunov‐projection method. However, substantial changes are made so that this algorithm is capable of solving the ALE form of incompressible Navier–Stokes equations. Multi‐block structured grids are used to discretize the flow domains. The grid velocity is not explicitly computed; instead the volume change is used to account for the effect of grid movement. A new method is also proposed to compute the freestream capturing metrics so that the geometric conservation law (GCL) can be satisfied exactly in this algorithm. This projection method is also parallelized so that the state of the art high performance computers can be used to match the computation cost associated with the moving grid calculations. Several test cases are solved to verify the performance of this moving‐grid projection method. Copyright © 2004 John Wiley Sons, Ltd. 相似文献