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In this paper we systematically investigate the influence of control parameters on the competition results between spiral waves and target waves. Driving frequency f , amplitude A and injection area n of the input signals are three important parameters and the competition results between spiral waves and target waves are influenced by these three parameters remarkably. Based on these understandings we can control spiral waves effectively by suitable combination these parameters to generate faster target waves. And the effective controllable parameter regions are also studied. 相似文献
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合成了一种新显色剂1-(4-硝基苯基)-3-(4,6-二甲基-2-嘧啶)-三氮烯(简称NPDMPMT),并研究了在非离子型表面活性剂Triton X-100存在下,于pH为11.0的Na2B4O7-NaOH缓冲溶液中与锌(Ⅱ)的显色反应.结果表明.Zn与试剂NPDMPMT形成1:2的橙黄色配合物,在456nm处有一最大正吸收,在530nm处有一最大负吸收,建立以530nm为参比波长,456nm为测量波长的双峰双波长测定法,其表观摩尔吸光系数为3.16×105L·mol-1·cm-1,锌(Ⅱ)浓度在0-8.0μg/25mL范围内符合比耳定律.方法用于人发中微量锌的测定,结果令人满意. 相似文献
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本文报道了在硫酸性介质中 ,以吐温 - 80为增溶剂 ,溴酸钾氧化姜黄催化光度法测定痕量钒 ( )的新体系。方法的检出限为 2 .6× 10 -3mg· L-1;相对标准偏差为 2 .7% (n=9) ,线性范围为 0 .0 12— 0 .0 4 0mg· L-1。可用于测定水样中痕量钒 ( ) ,结果满意 相似文献
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采用能带论中线性Muffin-tin轨道方法,计算了NdFe10M2(M=Ti,V,Cr,Mn,Mo,W)及渗N和C原子后材料的电子结构,得到了相应的总体态密度和各晶位的局域态密度,并由净自旋数得出了相应的磁矩及其变化,计算值与实验值相符合。 相似文献
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1-(4-硝基苯基)-3-(2-吡嗪)-三氮烯的合成及与镉(Ⅱ)的显色反应 总被引:1,自引:0,他引:1
报道了显色剂1-(4-硝基苯基)-3-(2-吡嗪)-三氮烯化合物的合成及其与镉(Ⅱ)的显色反应。在非离子表面活性剂Triton X-100存在下,pH 10.5的Na2B4O7-NaOH的缓冲介质中,该试剂能与镉(Ⅱ)与发生显色反应,形成摩尔比为4∶1的黄棕色配合物,配合物在波长453 nm处有最大吸收峰,表观摩尔吸光系数ε为6.90×104L.mol-1.cm-1,镉(Ⅱ)质量浓度在0~0.56μg/mL范围内遵守比尔定律。用拟定方法测不同废水中的镉(Ⅱ)。 相似文献
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A 1.3-μm wavelength vertical-mesa ridge waveguide mulitple-quantum-well (MQW) distributed feedback (DFB) laser with high directly modulated bandwidth and wide operation temperature range is reported. With the optimization of the strained-layer MQWs in the active region, the surrounding graded-index separated-confinement-heterostructure waveguide layers, together with the optimization of the detuning and coupling coefficient of the DFB grating, high directly modulation bandwidth of 16 GHz at room temperature and wide working temperature range from -40 to 85 ℃ are obtained. The mean time to failure (MTTF) is estimated to be over 2×10^6 h. The device is suitable as light source of high-bit-rate optical transmitters with small size and reduced cost. 相似文献
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