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
Suppose that any figure HGI is to be transformed. Draw, at pleasure,
two parallel lines AO, BL, cutting any third line AB, given by
position, in A and B, and from any point G of the figure, draw out any
right line GD, parallel to OA, till it meet the right line AB. Then
from any given point O in the line OA, draw to the point D the right
line OD, meeting BL in d; and from the point of concourse raise
the right line dg containing any given angle with the right line
BL, and having such ratio to Od as DG has to OD; and g
will be the point in the new figure hgi, corresponding to the
point G. And in like manner the several points of the first figure will
give as many correspondent points of the new figure. If we therefore
conceive the point G to be carried along by a continual motion through
all the points of the first figure, the point g will be likewise
carried along by a continual motion through all the points of the new
figure, and describe the same. For distinction's sake, let us call DG
the first ordinate, dg the new ordinate, AD the first abscissa,
ad the new abscissa; O the pole, OD the abscinding radius, OA
the first ordinate radius, and Oa (by which the parallelogram
OABa is completed) the new ordinate radius.
I say, then, that if the point G is placed in a right line given by
position, the point g will be also placed in a right line
given by position. If the point G is placed in a conic section, the
point g will be likewise placed[Pg 142] in a conic section. And here
I understand the circle as one of the conic sections. But farther, if
the point G is placed in a line of the third analytical order, the
point g will also be placed in a line of the third order, and so
on in curve lines of higher orders. The two lines in which the points
G, g, are placed, will be always of the same analytical order.
For as ad is to OA, so are Od to OD, dg to DG,
and AB to AD; and therefore AD is equal to ,
and DG equal to .
Now if the point G is placed in a right line, and therefore, in any
equation by which the relation between the abscissa AD and the ordinate
GD is expressed, those indetermined lines AD and DG rise no higher
than to one dimension, by writing this equation
in place of AD, and
in place of DG, a new equation
will be produced, in which the new abscissa ad and new ordinate
dg rise only to one dimension; and which therefore must denote
a right line. But if AD and DG (or either of them) had risen to two
dimensions in the first equation, ad and dg would
likewise have risen to two dimensions in the second equation. And so
on in three or more dimensions. The indetermined lines, ad,
dg in the second equation, and AD, DG, in the first, will always
rise to the same number of dimensions; and therefore the lines in which
the points G, g, are placed are of the same analytical order.
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