A Treatise on the Theory of Screws
Forfatter: Sir Robert Stawell Ball
År: 1900
Forlag: The University Press
Sted: Cambride
Sider: 544
UDK: 531.1
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436 THE THEORY OF SCREWS. [400
ordinates of the originating objects as constant, and regard the intervene
simply as a function of X and p, which we shall denote by /(X, p).
The form of this function will be gradually evolved, as we endow it with
the attributes we desire it to possess. The first step will be to take a third
object on the same range for which the parameter shall be v, where X, p, v
are arranged in order of magnitude. Then, as we wish the intervene to
possess the property specified in Axiom i,, we have
/(X, p) +f(p, v) =f(X, v).
By the absence of p from the right-hand side, we conclude that p must
disappear identically from the left-hand side. This must be the case
whatever X and t> may be. Hence, no term in which p enters can have
X as a factor. It follows that f(X,p) must be simply the difference of two
parts, one being a function of X, and the other the same function of p.
Accordingly, we write,
The first step in the determination of the intervene function has thus been
taken. But the form of </> is still quite arbitrary.
The rank of the objects in a range may be concisely defined by the
magnitudes of their corresponding values of p. Three objects are said to be
ordered when the corresponding values of p are arranged in ascending or descend-
ing magnitude.
Let P, Q, Q be three ordered objects, then it is generally impossible
that the intervenes PQ and PQ' shall be equal; for, suppose them to be so,
then
PQ + QQ' = PQ' by Axiom I.;
but, by hypothesis, PQ = PQf
and hence QQ’ — o.
But, from Axiom n., it follows that (Q and Q' being different) this cannot be
true, unless in the very peculiar case in which the intervene between every
pair of objects on the range is zero. Omitting this exception, to which we
shall subsequently return, we see that PQ and PQ' cannot be equal so long
as Q and Q' are distinct.
We hence draw the important conclusion that there is for each object P
but a single object Q, which is at a stated intervene therefrom.
Fixing our attention on some definite value S (what value it does not
matter) of the intervene, we can, from each object X, have an ordered equi-
intervene object p determined. Each X will define one p. Each p will
correspond to one X. The values of X with the correlated values of p form
two homographic systems. The relation between X and p depends, of course,