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SOLUTIONS OF A SMITH’S PRIZE PAPER FOR 1871.
511
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10. An endless heavy chain of given length is suspended from two fixed points in the
same horizontal plane: show that (.subject to a condition as to the length) the figure of
equilibrium may consist of portions of two distinct catenaries.
The two parts of the chain will each of them be a portion of a catenary, viz.
they will either coincide with each other, forming a twice repeated portion of a
catenary (which is always a possible position of equilibrium), or they will form portions
of two distinct catenaries. That the latter form is in some cases possible, appears
from the case of a very long chain. It is then clear that there is a position of
equilibrium in which the upper catenary is nearly a straight line. It may be added,
that, as the length of the chain diminishes, the two distinct catenaries approach more
and more, and for a certain value of the length become coincident; for any smaller
value of the length, the only position is that consisting of a twice repeated portion
of a catenary. But to obtain the solution in a regular manner, observe that, in order
to the existence of such a form of equilibrium, the necessary condition is, that the
tension at A (or B) must be equal in the two catenaries. Now the tension at any
point of a catenary is proportional to the height above the directrix of the catenary;
hence the condition is, that there shall be through the points A, B two catenaries having
the same directrix, and such that the sum of the lengths is equal to the given length
of the chain.
Take AB = 2a, the length of the chain = 21. Take /3 for the distance of the
directrix below the points A, B; c for the parameter of the catenary (or distance of
its lowest point above the directrix), /3, c being of course unknown. Then taking the
origin at the mid-point of the directrix, and the axis of y vertically upwards, the
equation of the catenary is
whence for the point A or B,
a a
/3 = l(e-° + e~°),
and the arc measured from the lowest point is
Hence, assuming that there are two distinct catenaries, if the parameters are c, c', we
have
a
a
a
a
%c(e c + e c ) = \c' (e c ' + e c '),
a
a
a a
%c (e c — e c ) + \c' (e
which are the conditions for the determination of c, c' ; and it is to be shown that
these can be satisfied otherwise than by taking c = c'.