989 resultados para RESONANCE-SPECTRUM


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Recent papers provide detailed analyses of more than 40 high-resolution time series culled from the extensive paleoclimate literature that appear to define cyclical elements of the Solar-Insolation/Tidal-Resonance Climate Model. This model was earlier referred to as the Milankovitch/Pettersson Climatic Theory. This paper provides comparable analyses of an additional 20 or so, evidently supportive, climate and volcanic time series. The tree-ring, historical, pollen, cultural, time-frequency, and hydrologic records range in length from 400 to 90,000 years and spatially from Alaska to Tierra del Fuego.

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The internal structure of rain falls in terms of rain rate during various instances of time can be determined by measuring rain amounts received during very short intervals of time. A system that can record the intensity of rain fall at every minute has been used for this study.

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应用改进DEAE-Toyopearl 650S阴离子交换柱层析从高等植物菠菜(Spinacia oleracea)中分离纯化了核心天线复合物CP43和CP47。并对它们的纯度和完整性色素种类和含量,以及色素分子的结合状态进行了研究并对色素分子间的能量传递机制进行了讨论。结果如下: 1、HPLC检测结果表明:纯化的CP43和CP47均只含Chla和β-Car两种色素分子,并且,平均每分子CP43多肽含19-20分子Chla和4-5分子β-Car;而平均每分CP47则含20-21分子Chla和3-4分子β-Car。 2、以436nm和480nm激发光激发样品得到的CP43和CP47的低温荧光发射光谱的最大荧光发射峰分别位于683nm和693nm。进一步发现,CP43和CP47,在相同条件下分别以436nm和480nm激发光激发样品得到的低温荧光发射光谱经归一化后几乎完全重叠,而且400-500nm波长范围内的激发光扫描得到的三维低温荧光发射光谱沿激发轴具有较好的对应关系,表明纯化的CP43和CP47都具有较高的完整性。 3、纯化的CP43和CP47的吸收光谱的红区最大吸收峰分别位于671nm和674nm。该光区的导数光谱均分辨出偏蓝区和偏红区两个子峰,CP43的这两个子峰分别位于669nm和682nm;而CP47的两个子峰则分别位于669nm和680nm。进一步用包含这两个子峰的高斯解析参数对红区最大吸收峰进行拟合,结果证明,拟合的曲线与实测曲线几乎完全吻合,这表明,CP43和CP47均至少包含两种不同状态的Chla分子。 3.1应用不同的变性温度处理CP43,发现随变性温度的不断提高,其红区最大吸收峰的峰值逐渐减小,四阶导数光谱分辨出的两个子峰同时减小,但差光谱显示:随处理温度的不断提高,这两个组分峰值的变化并不同步进行,较低温度范围内(55℃以下)682nm吸收峰下降明显,而较高温度范围内(55℃以上),669nm吸收峰下降明显。 同时,随处理温度不断提高CP43脱辅基蛋白的结构也在不断发生变化,其变化过程明显表现出两个跃变阶段。这两个跃变阶段分别出现在40~50℃范围内和55~60℃范围内,恰与吸收光谱两个组分峰变化的转变过程相一致。这证明,CP43中分别位于669nm和682nm的不同的色谱组分即代表两种不同结合态的Chla分子,分别简称为“CP43-669”和“CP43-682”。它们在色素蛋白复合物中所处的环境不同,因而对蛋白质结构的依赖性不同,前者更高地依赖于蛋白复合物的整体构象,而后者则主要依赖于蛋白质的二级结构。 3.2 经不同的变性温度处理的CP47,其红区最大吸收峰的峰位逐渐蓝移,而吸收峰值无明显的变化,只有当处理温度提高到65℃以后,蓝移后的吸收峰值(669nm)才开始明显减小;四阶导数光谱表现为680nm吸收峰的信号逐渐下降669nm的吸收信号逐渐明显;处理减对照差光谱只观察到680nm吸收值的逐渐减少,而几乎观察不到669nm吸收值的变化。同时,随变性温度的不断提高,CP47的脱辅基蛋白的结构也发生相应的变化与CP43不同,蛋白结构变化最大的温度范围为60℃~65℃之间,但同CP47的峰位蓝移、导数光谱中680nm信号的减小,以及差光谱中680nm吸收值的减小相一致。由此认为,同CP43一样,CP47的吸收光谱中分辨出的分别位于669nm和680nm处的两个不同光谱组分亦分别代表两种不同结合状态的Chla分子,分别简称为“CP47-669”和“CP47-680”,与CP43中的相应组分对应,它们处于不同的蛋白环境中,从而对蛋白质结构变化的依赖性不同。 3.3 CP43和CP47的CD光谱表现出明显的正负双峰,表明色素分子间存在较强的激子相互作用。随变性温度的不断提高,正负CD双峰的信号逐渐减弱,变化过程与脱辅基蛋白结构的变化以及CP43-682的变化相一致,表明色素分子间的激子相互作用更高依赖于CP43-682和CP47-680。并认为CP43-682和CP47-680可能以二聚体或多聚体的形式存在,并且二聚体或多聚体的形成依赖于蛋白天然构象。而CP43-669和CP47-669则以单体的形式位于蛋白结构中相对伸展的区域。并提出:在CP43-682以CP47-680分子之间,激发能主要以激子偶合机制进行而在CP43-669,CP47-669分子间及CP43-669至CP43-682间,CP47-669至CP47-680之间激发能则主要以Foster机制进行。 4、以488nm激发光得到的CP43和CP47的共振拉曼光谱都具有全反式构型类胡萝卜素分子的四个典型特征峰由此认为CP43和CP47中的β-Car分子亦具有全反式构型;与溶于丙酮抽体物中的β-Car分子相比较,CP43和CP47中的β-Car分子的共振拉曼光谱中具有较强的960cm~(-1)的拉曼峰,表明,CP43和CP47中的β-Car分子具有扭曲的构象。 应用经归一化后的吸收光谱与荧光激发光谱相比较的办法发现CP43和CP47中存在β-Car分子和Chla分子间的能量传递其能量传递效率分别为29.8~29.9%和52.3~56.9%。这表明,在正常条件下,CP47中β-Car分子和Chla分子间的能量传递效率远大于CP43。此外,当选用蛋白结构变化最明显的热变性温度处理样品后,发现,不论CP43还是CP47中β-Car与Chla分子间的能量传递效率大大降低,表明,这两种色素分子间的能量传递严格依赖于蛋白复合物的天然构象,并认为,正常条件下,CP43和CP47内β-Car与Chla分子间的空间距离较近,可能不大于10A,CP43和CP47相比较,CP47内这两种色素分子间的距离更近。并进一步提出,在CP43和CP47中,β-Car到Chla分子间的能量传递最大可能以Dexter的电子交换机制进行。

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In a surface stabilized ferroelectric liquid crystal cell, optical transmission oscillations have been revealed accompanying mechanical vibrations caused by fast field reversal. Special bookshelf textures, so-called "rainbow", were used in the experiments. Temperature dependences of the oscillation parameters have been studied. The temperature dependence of the oscillation frequency suggests that the some oscillation resonances correspond to modes of the liquid crystals.

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Carbon nanotubes (CNTs) have good mechanical properties and unique structural, electronic, thermal, and optical characteristics. In this work, we present the results of our investigations of a resonator device based on embedded vertical CNT arrays. The device's design is based on the mechanical resonance of the tubes. CoventorWare FEA tools have been used to simulate the mechanical resonance frequencies of the vertical nanotubes arrays integrated on a silicon substrate. ©2008 IEEE.

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It is known theoretically [1-3] that infinitely long fluid loaded plates in mean flow exhibit a range of unusual phenomena in the 'long time' limit. These include convective instability, absolute instability and negative energy waves which are destabilized by dissipation. However, structures are necessarily of finite length and may have discontinuities. Moreover, linear instability waves can only grow over a limited number of cycles before non-linear effects become dominant. We have undertaken an analytical and computational study to investigate the response of finite, discontinuous plates to ascertain if these unusual effects might be realized in practice. Analytically, we take a "wave scattering" [2,4] - as opposed to a "modal superposition" [5] - view of the fluttering plate problem. First, we solve for the scattering coefficients of localized plate discontinuities and identify a range of parameter space, well outside the convective instability regime, where over-scattering or amplified reflection/transmission occurs. These are scattering processes that draw energy from the mean flow into the plate. Next, we use the Wiener-Hopf technique to solve for the scattering coefficients from the leading and trailing edges of a baffled plate. Finally, we construct the response of a finite, baffled plate by a superposition of infinite plate propagating waves continuously scattering off the plate ends and solve for the unstable resonance frequencies and temporal growth rates for long plates. We present a comparison between our computational results and the infinite plate theory. In particular, the resonance response of a moderately sized plate is shown to be in excellent agreement with our long plate analytical predictions. Copyright © 2010 by ASME.

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http://www-civ.eng.cam.ac.uk/cjb/papers/cp88.pdf