Band 
Vol. II.
Seite
463
JPEG-Download
 

FLUXIONS.

40 ;]

b x

Second Form. The fluent of -

vV ±« 2

rithm of X -f- •/x-^a\

Third Form. The fluent of •

bi

is b X hyperbolic loga-

is b x hyperbolic loga-

s/ 2 a x x 1

rithm of a + x -f- f<> a x a 2 .

2 a b x

Fourth Form. The fluent of-■—■— is b X hyperbolic lo-

a — f a? ± x !

x s^a- ^ a-

garithm of •

a 4* V*" a- dt a ;

5. Certain fluents may be found by means of circular arcs of acircle to the radius 1.

Let AD, fig. 15, be a circular arc, put AT, its tangent = t, DBthe sine — y, AB = x, C’l = .r, the radius CD = a, and the arcAD — z\ also let lire tangent D s represent is, D n parallel toAB, s 7i to DB uill express .v andy. Then from the similar tri-

a 3 i ay

angles TAG, DBC, and D n s, we obtain x =

“ 5 + f J f u i

-, and thus four forms of fluxions,V 2 a a — a- VV — a 2

which diflVr only in the signs from those found by logarithms,}uay be found by means of circular arcs, whose lengths are givenhi a table, to a circle,,the radius of which is 1, thus,

bat t

First Form. The fluent of- — b X arc to tang. —.

a 2 i l a

by y

Second Form. The fluent of-= } X arc to sine—.

Third Form. The fluent of ■

S' a*—ifbx

b x arc to vers.

■/ I'm —x 1 0

bus r s

Fourth Form. The fluent of-= b x arc to see. —.

V s l —

T ° the above we add the following, which are easily investigated;the hyperbolic logarithm is to be understood, anti the radius of• the circle is 1.

-ORMS.

Fluxions.

II.

III.

IV.

Fluents.

ii— 1 .

«±c"

i — logarithm of a± x nn

— l

a±x*

An— i

a — x n

An — 1

« + x*

1 xn

— logarithm of-

no. a±^x n

1 fa -{- f x n

■ logarithm of ■

nf a

fa — fx n

1 a — x”

- X arc to cosine --

nfa « + *"

Forms.

V.

VI.

VII.

Fluxions.

Xr)_ 1

l x

f

An— 1

fa— x«

xf2ax—x?

Fluents.

— logarithm of f x n -{- f± a + x»n

• \ X 1 "

arc to sine v —

■ circ. seg. to rad. a and vers, x

(40.) When the given fluxion is so complex that its fluent can-not be found by any of these means, it is then to he determinedby the method of infinite series; thus, expand the radical or frac-tion in the given fluxion by division, extraction of roots, thebinomial theorem, &c. and multiply the series by the fluxionalletter, if il had been left out in the operation, and such variablesimple factor as the given fluxional expression may contain ; thenfind the fluent of each term, by the foregoing rules for the fluentsrequired.

ax

Thus, if it were proposed to find the fluent of -, it be-

a — x

comes necessary to throw the fluxion into an infinite series, by

_ x.v :;-.v

dividing ax by a — x: thus, ax ■—a — x = .i -j- - -(~

a

-j-, Ac. Now the fluent of each term of this series,

i- i 3

may be found by the foregoing rules to be x -|-(-

2a

3a 3

4a 3

-, & c. Again, to approximate the fluent of -

u 2 —xT x x‘x

we first find the value of

r 2 ]!

expressed in a series to be

1 3a

-X .r 2 -\ -

2uc 8 <fi

4 ac 3

8a 3 c

Xi'-j-

oa

16c 7

I

1

I6«c 5

I6« 3 c 3

I6a s c

X x® -}-, &c. which value

being multiplied by x n x, and the fluent taken by the rules above

laid down, wc get

+

3a

8c s

«-f t x cjn+5

a .«+3

«+3

+

5 a

4ac 3 8a 3 c 16 c 7 lCac 5 !6aV i6a 5 c

n+7

+, &c.

(4l.) The fluent found from a given fluxion by the foregoingrules will frequently require a correction, for though a fluent canhave but one fluxion, yet a fluxion may have an infinite number

of