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5. To illustrate these definitions : Suppose a point m be conceived to move from the position A, and to generate a line AP, A P
P by a motion any how regulated; and suppose the celerity of the point m, at any position P, to be such, as would, if from thence it should become or continue uniform, be sufficient to cause the point to describe, or pass uniformly over, the distance Pp, in the given time allowed for the Auxion : then will the said line pp represent the fluxion of the fluent, or flowing line, AP, at that position. 6. Again, suppose the right
C line mn to move, from the position AB, continually parallel to itself, with any continued motion, so as to generate the fluent or A
PI flowing rectangle ABQP, while the point m describes the line AP: also, let the distance Pp be taken, as before, to express the fluxion of the line or base AP; and complete the rectangle P29p. Then, like as PP is the fluxion of the line AP, so is Pq the fuxion of the flowing parallelogram AQ; both these fluxions, or increments, being uniformly described in the same time. 7. In like manner, if the solid
R r AERP be conceived to be
generated by the plane PQR, moving B
9. from the position ABE, always parallel to itself, along the line AD; and if pp denote the fluxion of the line. AP: Then, like as the rectangle PQqp, or PQ x Pp, denotes the fluxion of the flowing rectangle ABQP, so also shall the fluxion of the variable solid, or prism ABERQP, be denoted by the prism PQRrap, or the plane PR X Pp. And, in both these last two cases, it appears that the fluxion of the generated rectangle, or prism, is equal to the product of the generating line, or plane, drawn into the fluxion of the line along which it moves.
8. Hitherto the generating line, or plane, has been con• sidered as of a constant and invariable magnitude; in which case the fluent, or quantity generated, is a rectangle, or a prism, the former being described by the motion of a line, and the latter by the motion of a plane. So, in like manner are other figures, whether plane or solid, conceived to be de
scribed by the motion of a Variable Magnitude, whether it be a line or a plane. Thus, let a variable line pe be carried by a parallel motion along ÁP; or while a point p is carried along, and describes the line AP, suppose another point
to be carried by a motion perpendicular to the former, and to describe the line pe: let pq be another position of PQ, indefinitely near to the former; and draw or parallel to Ap. Now in this case there are several fluents, or flowing quantities, with their respective fluxions: namely, the line or fluent AP, the fluxion of which is pp or Qr; the line or fluent PQ, the fluxion of which is
the curve or oblique line AQ, described by the oblique motion of the point Q, the fuxion of which is eq; and lastly, the surface APQ, described by the variable line PQ, the fluxion of which is the rectangle Porp, or PQ x Pp. In the same manner may any solid be conceived to be described, by the motion of a variable plane parallel to itself, substituting the variable plane for the variable line; in which case the Huxion of the solid, at any position, is represented by the variable plane, at that position, drawn into the fluxion of the line along which it is carried,
9. Hence then it follows in general, that the fluxion of any figure, whether plane or solid, at any position, is equal to the section of it, at that position, drawn into the fluxion of the axis, or line along which the variable section is supa posed to be perpendicularly carried ; that is, the fluxion of the figure app, is equal to the plane PQ X pp, when that figure is a solid, or to the ordinate PQ x Pp, when the figure is a surface.
10. It also follows from the same premises, that in any curve, or oblique line AQ, whose absciss is ap, and ordinate is PQ, the fluxions of these three form a small right-angled plane triangle ogr; for or = Pp is the fluxion of the absciss AP, qr the fluxion of the ordinate PQ, and eq the fluxion of the curve or right line AQ. And consequently that, in any curve, the square of the fluxion of the curve, is equal to the ,
sum of the squares of the fuxions of the absciss and ordinate, when these two are at right angles to each other.
11. From the premises it also appears, that contemporaneous fluents, or quantities that flow or increase together, which are always in a constant ratio to each other, have their fuxions also in the same constant ratio, at every position. For, let AP and BQ be two contemporaneous fluents, described in the same
P time by the motion of the points P and
А P the contemporaneous positions being P, Q, and poq; and let AP be to
Q 9 BQ, or Ap to B9, constantly in the ratio of 1 to n. Then
is n X AP = BQ,
and n x ap = Bq; therefore, by subtraction, n x Pp = 99. that is, the Auxion Pp: fuxion 09::1!, the same as the fluent AP : fluent BQ::1; ñ; or, the fluxions and fluents are in the same constant ratio.
But if the ratio of the fluents be variable, so will that of the fluxions be also, though not in the same variable ratio with the former, at every position.
12. To apply the foregoing principles to the determination of the fluxions of algebraic quantities, by means of which those of all other kinds are assigned, it will be necessary first to premise the notation commonly used in this science, with some observations. As, first, that the final letters of the alphabet x, y, x, 4, &c, are used to denote variable or flows ing quantities; and the initial letters a, b, c, d, &c, to denote constant or invariable ones: Thus, the variable base AP of the flowing rectangular figure ABQP, in art. 6, may be represented by *; and the invariable altitude PQ, by a: also, the variable base or absciss AP, of the figures in art. 8, may
be represented by x, the variable ordinate PQ, by y; and the variable curve or line ag, by z.
Secondly, that the fluxion of a quantity denoted by a single letter, is represented by the same letter with a point over it : Thus, the fluxion of x is expressed by *, the fluxion of y by j, and the fluxion of z by z. As to the fluxions of
ż constant or invariable quantities, as of a, b, c, &c, they are equal to nothing, because they do not flow or change their magnitude. VOL. II
Thirdly, that the increments of variable or flowing quantities, are also denoted by the same letters with a small' over them: Thus, the increments of x, y, %, are x', y, z:
13. From these notations, and the foregoing principles, the quantities, and their fuxions, there considered, will be denoted as below. Thus, in all the foregoing figures, put
the variable or flowing line : AP = *,
AQ = 2:
Pp the fluxion of the line AP,
ż = 99 = V(** + y) the fluxion of AQ; and
the constant generating plane PQR; also,
ni = Qq the fluxion of the same. 14. The principles and notation being now laid down, we may proceed to the practice and rules of this doctrine; which consists of two principal parts, called the Direct and Inverse Method of Fluxions ; namely, the direct method, which consists in finding the fluxion of any proposed fluent or flowing quantity; and the inverse method, which consists in finding the fluent of any proposed fluxion. As to the former of these two problems, it can always be determined, and that in finite algebraic terms; but the latter, or finding of fluents, can only be effected in some certain cases, except by means of infinite series. First then, of
THE DIRECT METHOD OF FLUXIONS.
To find the Fluxion of the Product or Rectangle of two Variable
Quantities. 15. Let ARQP, = xy, be the flowing or variable rectangle, generated R by two lines PQ and RQ, moving alwaysperpendicularto each other, from the positions ar and AP; denoting the one by x, and the other by y; supposing * and y to be so related, that the curve line AQ may always pass through the intersection e of those lines, or the opposite angle of the rectangle.
Now, the rectangle consists of the two trilinear spaces APQ, ARQ, of which, the
fluxion of the former is PQ X Pp, or gås
that of the latter is RQ X Rr, or xỳ, by art. 8; therefore the sum of the two soy + xy, is the fluxion of the whole rectangle xy or ARQP.
The Same Otherwise.
16. Let the sides of the rectangle x and y, by flowing, become x + x and y + ý: then the product of these two, or xy + xy + yx'+x'y will be the new or contemporaneous value of the flowing rectangle Pr or xy: subtract the one value from the other, and the remainder, xy + yx' + x'j, will be the increment generated in the same time as x' or y; of which the last term x's is nothing, or indefinitely small, in respect of the other two terms, because t' and ý are indefinitely small in respect of x and y; which term being therefore omitted, there remains xy + yx' for the value of the increment; and hence, by substituting * and j for x' and ý; to which they are proportional, there arises xy + you for the true value of the fluxion of xy; the same as before.
17. Hence may be easily derived the fluxion of the powers and products of any number of flowing or variable quantities whatever; as of xyz, or uxyz, or vuxyz, &c. And first, for the fluxion of xyz : put p = xy, and the whole given fluent xyz = 9, or q = xyz = pz. Then, taking the Auxions of q = pz, by the last article, they are q = pz + px; but p = xy, and so p = xy + xy by the same article; substituting therefore these values of p and j instead of them, in the value of q, this becomes q = xyz + xyz + xyż, 9
, the fluxion of xyz required; which is therefore equal to the sum of the products, arising from the fluxion of each letter, or quantity, multiplied by the product of the other two.
Again, to determine the fluxion of uxyz, the continual product of four variable quantities; put this product, namely uxyz, or qu = 1, where q = xyz as above. Then, taking the
= fluxions' by the last article, r = gu + qu; which, by substituting for q and a their values as above, becomes r = uxyz + uxyz + uxyz + uxyż, the fluxion of xyz as j
, required : consisting of the fluxion of each quantity, drawn into the products of the other three.