On the Motion of Paired Vortices with a Common Axis
On the Motion of Paired Vortices with a Common Axis
复制标题
关于共轴成对涡旋的运动
DOI:
10.1112/plms/s1-25.1.185
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发表时间:
1893
影响因子:
1.8
通讯作者:
A. Love
中科院分区:
文献类型:
--
作者:
A. Love
1. The investigation in this paper was undertaken with the view of throwing some further light on a problem in the motion of vortexrings which was first considered by Helmholtz in his original memoir on vortex-motion.* He found that two vortex-rings having the same axis and circulations in the same direction travel in the same direction parallel to the axis;" the foremost widens and travels more slowly, the pursuer shrinks and travels faster, till finally, if their velocities are not too different, it overtakes the first and penetrates it. Then the same game goes on in the opposite order, so that the rings pass through each other alternately." f It is extremely difficult to obtain a more detailed account of the motion here described." We are ignorant of the condition that the motion may be periodic, and we can only make guesses at the length of the period when the unknown condition is satisfied. Yet in applications of the vortex-atom theory to problems of radiation and chemical combination, it is conceivable that this period and the type of motion may play an important part. I propose here to imitate some of the circumstances of the problem by considering the case where there are present in an infinite fluid two pairs of cylindrical vortices of indefinitely small section, the circulations about the two vortices of each pair being equal and of opposite sign, the circulations about the four vortices being equal in absolute magnitude, and the line of symmetry for one pair coinciding with that for the other. A single pair of this kind moves parallel to the axis of symmetry with constant velocity. Two pairs with circulations in the proper directions influence each other's motions in a manner analogous to that exhibited by thin rings. I find a condition that the motion may be periodic, the length of the period, and the form of the curve described by one vortex of one pair relative to the homologous vortex of the other pair.