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Figuring the Acceleration of the Simple Pendulum

机译:计算简单摆的加速度

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摘要

The centripetal acceleration has been known since Huygens' (1659) and Newton's (1684) time.~(1,2) The physics to calculate the acceleration of a simple pendulum has been around for more than 300 years, and a fairly complete treatise has been given by C. Schwarz in this journal.~3 But sentences lik"the acceleration is always directed towards the equilibrium position" beside the picture of a swing on a circular arc can still be found in textbooks, as e.g. in Ref. 4. Vectors have been invented by Grassmann (1844)~5 and are conveniently used to describe the acceleration in curved orbits, but acceleration is more often treated as a scalar with or without sign, as the words acceleration/ deceleration suggest. The component tangential to the orbit is enough to deduce the period of the simple pendulum, but it is not enough to discuss the forces on the pendulum, as has been pointed out by Santos-Benito and A. Gras-Marti.6 A suitable way to address this problem is a nice figure with a catch for classroom discussions or homework. When I plotted the acceleration vectors of the simple pendulum in their proper positions, pictures as in Fig. 1 appeared on the screen. The endpoints of the acceleration vectors, if properly scaled, seemed to lie on a curve with a familiar shape: a cardioid. Is this true or just an illusion?
机译:自从惠更斯(1659)和牛顿(1684)时代以来就已经知道了向心加速度。〜(1,2)计算简单摆的加速度的物理学已有300多年的历史了,相当完整的论文已有〜3但是在教科书中仍然可以找到诸如“加速度总是指向平衡位置”之类的句子,例如在圆弧上的摆动图片旁边,例如在参考文献中4.向量是由格拉斯曼(Grassmann)(1844)〜5发明的,可以方便地用于描述弯曲轨道上的加速度,但是正如加速度/减速度一词所暗示的那样,加速度通常被视为带或不带符号的标量。切向分量足以推断出简单的钟摆周期,但不足以讨论钟摆上的力,正如Santos-Benito和A.Gras-Marti指出的那样。6一种合适的方法解决这个问题的方法很不错,可以用来进行课堂讨论或家庭作业。当我在其适当位置绘制简单摆的加速度矢量时,屏幕上将出现如图1所示的图片。如果正确缩放比例,加速度矢量的端点似乎位于曲线上,形状相似:心形。这是真实的还是只是幻想?

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