模拟链条滑出桌面

J. Vrbik
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引用次数: 0

摘要

考虑一条由n+ 1个相同质量的点状粒子(通过选择单位等于1)组成的链,由n个无质量的、完全灵活的、长度相等的非弹性链接(也等于1)连接。链放在桌面上,笔直且垂直于边缘。然后将第一个粒子(连同链的其余部分)轻轻拉过桌子的边缘。这导致链条开始向下滑动,由于重力(也是单位量级),以无摩擦的方式b[1]。现在让我们假设k个粒子已经离开了表格,它们的位置由k个角度j1, j2,…, jk,前k个连杆偏离垂直线的距离,s,最后一个粒子离开表边的距离(因此jk是相应连杆悬挂部分的角度;其余的仍然平躺在桌子上)。总的来说,这k + 1个变量被称为广义坐标[2],因为它们完全指定了每个粒子的位置。现在,使用直角坐标,原点在桌子的边缘,x轴垂直向下,y轴水平指向,远离桌子,我们可以计算出每个粒子对应的x和y坐标
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Simulating a Chain Sliding off a Desktop
Consider a chain consisting of n+ 1 point-like particles of the same mass (equal to 1, by a choice of units), connected by n massless, perfectly flexible, inelastic links of equal length (also equal to 1). The chain is laid on a table top, straight and perpendicular to the edge. Then the first particle is pulled (together with the rest of the chain) gently over the edge of the table. This causes the chain to start sliding down, due to gravity (also of unit magnitude), in a frictionless manner [1]. Let us assume now that k particles have already left the table, and that their positions are defined by k angles j1, j2, ..., jk by which the first k links deviate from the vertical, and by s, the distance of the last particle to have left the table edge (jk is thus the angle of the hanging part of the corresponding link; the rest of it still lies flat on the table). Collectively, these k + 1 variables are known as generalized coordinates [2], as they fully specify the position of every particle. Now, using rectangular coordinates with the origin at the table’s edge, the x axis oriented vertically downward, and the y axis pointing horizontally, away from the table, we can compute the corresponding x and y coordinates of each particle by
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