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在电磁学中 ,学生判断通电导线周围磁场方向的安培定则 (亦即右旋定则 )、判断通电导线所受磁场力方向的左手定则以及判断感应电流方向的右手定则 ,经常出现搞不清到底是用左手还是用右手 ,而“左手因果定则”可以很好地避免上述定则的缺憾 ,所谓“左手因果定则” ,就是四指指原因 ,拇指指结果 .学生在使用过程中也认为“左手因果定则”易记、易学、好用 .现将用该定则在判断磁场方向、通电导线的受力方向及感应电流的方向的具体作法介绍如下 :1 用“左手因果定则”判断磁场方向 在这里 ,电流是原因 ,磁场是结果 .1 .1 判断通电导线周… 相似文献
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一般电工人士认为用普通低压验电笔不能区分交直流和判断直流电正负极,其实是可以的.本文就介绍用低压验电笔区分交直流和判断直流电正负极的方法、原理. 相似文献
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针对指针式三用表易损坏,故障判断比较复杂、困难的特点,笔者在实践的基础上,从指针摆动情况与故障的联系入手,总结出只需观察指针摆动情况就能判断三用表故障的方法。 相似文献
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一些中学生在课外活动进行电子制作时,常苦于没有万用表,不能判断一些电子元件是否损坏.笔者用电子电路制作了一台简易电子元件测试仪,用它可以大致判断小电容、二极管、三极管和电子线路等是否损坏. 相似文献
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现行高中教材(必修)第二册第76页介绍的左手定则是用来判断安培力方向的.其内容为:"伸开左手,使大拇指跟其余四个手指垂直,并且都跟手掌在一个平面内,把手放入磁场中,让磁感线垂直穿过手心,并使伸开的四指指向电流的方向,那么,拇指所指的方向,就是通电导线在磁场中的受力方向."用这个方法判断导线的受力方向,确实很好.而且把磁场、电流、安培力三个物理量方向的关系,在一只手上表示出来,很方便.但是,我在多年的教学实践中,发现这个定则也有一些缺点.例如,有些时候由于方位的关系,左手用起来很别扭.当磁场的方向与电流的方向不垂直时,如何让磁感线垂直穿过手心,有些费解.在磁场和电磁感应这一段内容中有用右手判断电流的磁场方向的安培定则,有用右手判断感应电动势方向的右手定则,有用左手判断安培力的左手定则.什么时候用左手,什么时候用右手,有些学生分不太清楚.基于这些原因,我想能不能用其他的方法判断.经过分析探索,找到了一些简单易行的方法,向同行们介绍以求赐教. 相似文献
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一、引言Chauvenet 准则和 Laeda 准则,都是判断实验数据的异常值是否包含粗差的常用统计方法。可是,对同一个样本,这两种准则的判断结果却往往相反,例如,用 Cha-uvenet 准则去判断文献[1]、[2]中那些正态样本的异常值,均得出样本的其余观测值是来自一个正态母体,而样本的异常值却来自另一个正态母体;而用 Laeda 准则去判 相似文献
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成簇的微钙化点是早期乳腺癌的一个重要表征,用计算机辅助诊断时需要在乳腺片图像中判断有无钙化点簇。提出了一种利用Daubechies小波对乳腺图像进行增强,用二维熵阈值分割法对增强后的图像进行阈值分割,然后采用图论方法提取出成簇钙化点的方法。从而实现了计算机辅助诊断系统辅助医师判断恶性钙化。 相似文献
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产生感应电流的条件及感应电流方向的判断分为两种:闭合电路的部分导体在磁场中做切割磁感线运动,感应电流的方向用右手定则判断(初中教材);穿过闭合电路的磁通量发生变化,感应电流方向由楞次定律判断(高中教材).以上两种又概括为穿过闭合电路的磁通量发生变化.这样,感应电流的方向可统一来用楞次定律判断. 相似文献
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三波长分光光度法测定色氨酸、酪氨酸和苯丙氨酸的研究 总被引:5,自引:0,他引:5
本文用三波长分光光度法测定了色氨酸、酪氨酸和苯丙氨酸。利用计算机选择最佳波长组合,可实现三种组分的同时测定。合成样品的分析结果表明,方法的准确度和精密度都令人满意。 相似文献
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Jos Roberto Berretta Wagner de Rossi Maurício David Martins das Neves Ivan Alves de Almeida Nilson Dias Vieira Junior 《Optics and Lasers in Engineering》2007,45(9):960-966
The technique to weld AISI 304 stainless steel to AISI 420 stainless steel with a pulsed Nd:YAG laser has been investigated. The main objective of this study was to determine the influence of the laser beam position, with respect to the joint, on weld characteristics. Specimens were welded with the laser beam incident on the joint and moved 0.1 and 0.2 mm on either side of the joint. The joints were examined in an optical microscope for cracks, pores and to determine the weld geometry. The microstructure of the weld and the heat affected zones were observed in a scanning electron microscope. An energy dispersive spectrometer, coupled to the scanning electron microscope, was used to determine variations in (weight %) the main chemical elements across the fillet weld. Vickers microhardness testing and tensile testing were carried out to determine the mechanical properties of the weld. The results of the various tests and examinations enabled definition of the best position for the incident laser beam with respect to the joint, for welding together the two stainless steels. 相似文献
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A method is suggested to determine both the refractive index and the transverse sectional shape and area of fibres, having skin–core structure, at the same time for the same region of the fibre. The method depends on using a fibre rotator device attached with Pluta polarizing interference microscope, to record the variation of the fibre thickness at each angle of rotation. Nylon 6 fibres having skin–core structure were used in this study. Beck-line method was used to determine the refractive index of the skin for light vibrating parallel and perpendicular to the fibre axis. To confirm the results of the suggested method, the optical microscope was used to determine the transverse sectional shapes of bundles of nylon 6 fibres. The mean refractive indices of the skin and core of nylon 6 fibres were determined. Microinterferograms are given for illustration. 相似文献
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Current lattice Boltzmann methods for simulating two fluids create a diffuse interface between the fluids. In this work, we
develop a novel technique for embedding sharp interfaces between fluids with unbounded density ratios for the LB method. Distribution
functions streamed across an interface are transformed so that the receiving node is passed information corresponding to its
fluid phase. Two different methods are employed to determine the transformation. The first uses analytical distribution functions
from steady Poiseuille flow to determine the jump in moments of the distribution functions across the interface. The second
uses approximate expansions of distribution functions to determine jumps in distribution functions. The accuracy and stability
of the methods are examined in simulations of Poiseuille-Couette flows with an interface parallel to the walls. Both methods
show linear convergence to the analytical solution. 相似文献
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A model describing ray propagation in both the core and cladding regions of a multimode optical fibre is developed. This model is then used to determine the influence of the fibre outer protective sheath on far-field measurements and to determine the equilibrium source conditions for the modified near-field technique. 相似文献
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通过EC法与FP法的混合定量分析方法,建立了用于微球壳层掺杂元素含量测量的校准模型;基于对微球直径、PS、PVA层厚度对分析元素荧光强度影响的理论计算及XRF实验研究,将该模型用于ICF微球壳层掺溴含量的测量,得到微球壳层掺溴含量较为精确的分析结果,实验结果表明:XRF法测量ICF微球壳层掺溴含量具有较高的精度,在微球涂层厚度大于10 μm时,其测量相对误差在5%左右。 相似文献