60 7 )
F
L
u
x
F
~
LU:CroNS,
a metltod of eakulation whieh great ly
t:t:dit.Hes eorr.p"tlt'ons in lhe
I,,~hcr
pms oi'
011'
Ihc01Jlics. Sir Ir.I..,c N(WIOnand Mr Lribnilz coJltend ·
ed fur the Itnnour of inveming it
It
's
rroba~¡(
they
¡,Id both maJe progref, in the lame d,CcoYtry. unknown
lO' ?eh olher, before there \Vas
~ny
publication on the
fubje[t,
In th i, branch of mathematics magnitudes of every
kinJ
m
fup?ofed genermd by motion: a I,ne by the
moti~n
of a point, a furf,cc by the motion of a line, "nd
?
fol,J by the mOtioDof a fu,fAce. And fome pan of
a
ligure is fuppofed gencrmd by an uniform motion; in
ronfequl nc~
of which the olher pans m"y increale uni·
formly l'r \Vith .n
a~cekrated
or warded motion, or lIlay
r.medfe in
a~y
of th,Ce ways; and the compu tations are
marlé by traciog lhe comparative veloeities with \Vhieh
t!::
pam
flo.·.
Fig. t. If lhepmlldogram AlleD be generated by
3n uoifo, m motion of lhe line AB tOI'.'..d CD whtlé
'1
mOl'eS from
FE
lowardsj(, \Vhik thelinefl Freeeiyes thein·
crement Ff, and the fig"re \ViII be ioereafed by the parolle.
logram
F,;
the line FE io this cafeundergoes 00 varialioD.
The Jluxioo of aoy m"goitude at aoyPOiDt is the inere·
meot that it 1V0uld receiye in anygiven time, Cuppofing it
toinmaCe uniformly fromtha! point ; and as the mea·
fure, ..ill be the fame, whatever the time be, \Ve are al
liberty to fuppoCe it
I<C¡
thanan)' afligned time.
Tt!e firn leners in the alphdbet are ufed to reprefent
,nvan,ble quantities; the lener,
x,
J,
z
vari.ble quanti.
ties; and the fame Imers with points over them ;,
j,
;,
reprefent their
ftuxio~.
Thtrtfore if
A
3=11,
an¿ EF=x ;
Ff,
the fl uxioo of
BF,
wiU be= ; , and F" the Rnxion of AF,
=11;.
I ~
the re.'langle be fuppoféd geomted by the onlform
mouon of fe
tO..
~rds
eD,
at the fame time He moyes
unifo;mly
tOwarJ.
AD, thé point
G
Iteeping always on
thedtagooal, ,he lines fe
HG
IVill fiolV unifo,mly,; for
"'h,le B/ ,mires the inCrentént
FI
and HIJ , the incre·
~e,nt
IIK, FG
\ViII receiye the incremem
hg
and HG the
lnerement
hl(.
and they wdl receive equal iocrements in
e~ual
fueeelhe times. But the paralldogram will fiolV
W'th ao aeceler:ued motÍon; for while F flows tO
I
and
J!
to
K,
it i, increafeel by the gnomoo
Ke/:
but while
~
30d
rr
fio\\'
throu~h
the equal fpaces
1m
K1,
it is io·
~reared
by the
~OOO1en
LglII
gremr thdO Ke( ; confe–
queotl~
IVhen Ru.ioos of the fi des of a p",tllelogram
are uOlform, the flux,on of the pJr.Ile1ogram
,ncrcal~s
t.Onunu:<lIy.
The
fic~ion
(lf the pmllrlogmn BHeF is the tIVO
pmUdograms
KG
and
Gf;
fur th, u;:h the pu nolcte,
reeCilrs ao increment of the I!nOnt1'l1
KG!.
IVI"le its
~dlS
fiolV to
I
and
K,
the pm
xC
IS ou',ng to the addi-
1I00:,j
vellllity whe'ewlth
1111
r"'dl~dl)gr;:m ilow~
clur:ng
that,IImr; ano thc"f",c i, no I,;r' nf the meaf"r. of the
ft
JX'OO, wlnd,
mlla
~c
CUtllputCU
uy
r"l'l'of:ng the rar,t·
1
o
s.
meter to flow ttn:fo rn,ly as it oiJ at the beginning, witl.·
OUt auy acceler.tioo.
ThLfefure if the fiJ,s of
a
paraJ!c1ogram be
x
and
J,
théir fluxions wiUbe
.~
):; and the flu xion of the pa·
t.J1elogfdm
xj+J;:
and if
x=)',
that ¡s, if the figure be a
fq u,tre, the Bux,on of
r'
will be
2X;.
FiC'
2.
Let the ttiangle ABC be dcrctibcd by the
unifurm mo:ioo of
DE
from
A
tOlVards
B,
the point
E
moying in the line DF, fo dS dIVays to toueh the lines
AC, CH; while D moves from Ato F, DE is uniform–
Iy increafed, aod the inereafe of the triangle is uniform–
Iyaec/bated. When
VE
is in the polition FC, it is
a maximum. As D moy/s from F
tu
B,
the line
n:
decreares, and the triaeg!e ,ocréafes, but with a motion
unifonnly retardcd.
Fig
3.
Ir
the femicircle AFB be geoeraleo by the
uniform motionof CD f,om
A
toward.
B.
while Cmoves
fro",
¡\
tO G, the line CD wiJl increare, but \Vitn are·
tarded motion: the circumfertnce alfo incre,fes with a
ret~rrlcd
motion, aod tbt circular fpace increafes
~'ith
an
accdeldted motlon, but not unifo,dy, the degtee. of
acrelcrationgro.,ing Itfs as CD approache, tO the pofitioo
GF. Wheo e moyes from
G
tO
(J ,
it decreafes \Vitl¡
a motion cominually aecclerated, the circumfmnce in–
creafes IVilh a motion continually aecelerated, aod the
area increafes \Vith a motion cominually rrtarded, and
more
quic~ly
retarded as CD approaches to B.
The fluxion of a quaotity which decre, fes
is
tObe con-
fidereJ as negatiye.
.
When a quantity does not fio\V uniformly, its fl uxioD
may bereprefented by avariable quantity, or a line of
a
."riable léog'o; the Ruxion of fu h a I,ne is eaJled the
ftcond fiux,on of the quantity " hofe fiuxion tbat line is:
and if it be variable, a third flnxion m"y be dedueed from
it,.and higher order! from th& in the fdme manae': the
Ctcond flux ion is rep" rcnr"d by t\Vo poiots, as ; .
The increment a quanttty receives by flowing for any
gi"en time, contaios meafurtl of all tht ddrérent order!
01' flux,ons ; for if it incré,les unifotmly, the whole in–
errmen! is the hrfl fiuxion; and it h"s no fecond IIltx:oo.
If it incre" frs with a motion u",fonnly ,ccebateel, the
palt oi' the ,ncrement oceafi"ned by th, (,rll motion mea·
fUlcl tile r,rn lIuxion, and the par! occafioo,d by the ac·
rder.tion mcafurcs thc I.c,,"d fl,Ixion.
[1'
the mvtion
~c
not ollly accdératrd, but thé degree of aCederation
continu. lly increafrd, the't\Vo lira fiU XlllOS are me"lur,tI
as betore; aoJ rhe par! of the inen
ment
occafioncd hy
tite additillnal degrce uf accdrratioo me"furc) the th"d ;
aotl
r"
on
Thde rr.cafi,rt! rcqll" e tO be (lI"céted, antl
Jre only mention,d hae tO tllullrm thefubj<éL
D I R E CT
~I
ET
JI
O D,
AnJ JI,..I
¡,\~
q/ldr.titJ b,'ing git:n,
ID
pntl itl JI:/xi ,n.
R
oU
1.
To finu tite fiuxiun of any pOll'cr of a qUJn.
titi