Newton's Principia : $b The mathematical principles of natural philosophyNewton, Isaac
General
Newton's Principia : $b The mathematical principles of natural philosophy
Newton, Isaac
Celestial mechanics -- Early works to 1800; Mechanics -- Early works to 1800
Wherefore the sense of the Lemma is, that if the moments of any
quantities A, B, C, &c., increasing or decreasing by a perpetual
flux, or the velocities of the mutations which are proportional
to them, be called a, b, c, &c., the moment
or mutation of the generated rectangle AB will be aB +
bA; the moment of the generated content ABC will be aBC
+ bAC + cAB; and the moments of the generated
powers , , ,
, ,
, ,
, ,
will be 2aA, ,
, ,
,
,
, ,
,
respectively; and, in general, that the moment of
any power , will be
. Also, that the
moment of the generated quantity
will be ; the moment of the
generated quantity will be
;
and the moment of the generated quantity or
will be
;
and so on. The Lemma is thus demonstrated.
CASE 1. Any rectangle, as AB, augmented by a perpetual flux, when,
as yet, there wanted of the sides A and B half their moments
and , was
into , or
; but
as soon as the sides A and B are augmented by the other half moments,
the rectangle becomes into ,
or .
From this rectangle subduct the former rectangle, and there will remain
the excess aB + bA. Therefore with the whole increments
a and b of the sides, the increment aB + bA
of the rectangle is generated. Q.E.D.
CASE 2. Suppose AB always equal to G, and then the moment of the
content ABC or GC (by Case 1) will be gC + cG, that is
(putting AB and aB + bA for G and g), aBC
+ bAC + cAB. And the reasoning is the same for contents
under ever so many sides. Q.E.D.
CASE 3. Suppose the sides A, B, and C, to be always equal among
themselves; and the moment aB + bA, of ,
that is, of the rectangle AB, will be 2aA; and the moment
aBC + bAC + cAB of , that is, of
the content ABC, will be . And by the same reasoning
the moment of any power is .
Q.E.D.
CASE 4. Therefore since into A is 1, the
moment of drawn into[Pg 263] A, together with
drawn into a, will be the moment of
1, that is, nothing. Therefore the moment of ,
or of , is . And
generally since into
is 1, the moment of drawn into
together with into
will be nothing. And, therefore, the moment
of or will be
. Q.E.D.
CASE 5. And since into
is , the
moment of drawn into
will be a (by Case 3);
and, therefore, the moment of
will be or
. And, generally,
putting equal to ,
then will be equal to , and
therefore equal to ,
and equal to ,
or ; and therefore
is equal to b,
that is, equal to the moment of . Q.E.D.
CASE 6. Therefore the moment of any generated quantity
is the moment of drawn
into , together with the moment of
drawn into , that is,
;
and that whether the indices m and n of the powers be
whole numbers or fractions, affirmative or negative. And the reasoning
is the same for contents under more powers. Q.E.D.
Public-domain text, read in full here on John Shaqi.
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