M
E
e
H
ue.
and conf:quently, the whole (paces areas [he fqu ares
of lhe t:lllo.!S, ur uf
,he lan acquired
veJociries.
r'or
J
,rht.: continucl.l ilddition of (he odd
AU Lnbers
yitlds
,he
fquares of all
num~ers
[rom un¡ty upwards. Thus,
1,
is lhe
firn
odd nUnlher, and
,he
fqu are of
1
is
1;
3
¡so
the (econd odJ number, and lhis added
{Q
I
makes 4,
,he
fqul rl! of 2;
5
IS lhe
thirJ odd number. which added
tO
4
mAkcs
9, tbe
fqudre
of 3 ; and fa on for ever. Sioce,
thercfore, lhe times aad
velocities
procecd
evenly
aDd
con!bntlyas
1, 2,
3 4,
&c
but ,he Cpaces deCcribed
io each equal time élre as
I,
3, S'
7.
Cc.
it
is e,·ident
thar ,he Cpaee deCcribed,
In
1
minute will be -
1
=
Cquare of
1
I n
2
mmu ,es - -
1+3=
4
=
Cqua« of
2
In
3.
mlnu'es -
1+3+S=
9
=
C'luare of 3
In 4 minutes
1+3+5+7=16 =
Cquare of 4 &c_
A s heavy bodies are uniformly
accderated
by
lile power
of gravity in their
deCcent, it is plain
chac
they muO:
be uniformly rctarded by the fame power
in
their af–
cent. Thuefore, the velocity which a body acquires by
f,dling. is fufficient tO carry it up again tO lhe fame
h eigi: t (rom whence il felJ; alJowance beiog made for
the refil1ance of the air, or other medium in which lhe
body is moved_ Thus, Ihe body D (lig.
2_)
in rolling
dOWD
the inclined plane
AB,
will acquire fuch a velocity
by
lhe
time
it
arrlves al
B,
as
wilI
carry it up to the io–
c1ined plane
BC,
almo!l to
C;
aod would carry it quite
up 'o C, if the body and plane \Vere perfeétly Cmooth,
and the air gave no
reCil1ance.~So,
if a pendulum were put
into motioo in a rpace quite void of air and all other re·
fillance, aod had no fr¡étion on lhe paint of fufpenGon, it
would move for ever; for the vclocity it had acquired in
falJing through lht! dt!rcending part of the are, would be
llilJ fufficient
lO
carry i, equalJyhigh in the afcending pan
thereof.
Th~
centre o/
gtavily
is that poinl of
a
body io which
the \Vhole force c.(its gravity or wc:ight is united. There–
fore, whatever fupports th.a point bectrs the wdght of the
whúle body; and whilfl i, is C"pponed, ,he body cannot
fati, becaufe all
in
pans are in a perfeét equilibriulIl
a·
bo"ut thac point.
An imaginary line drawn from the centre of gr;¡vity of
any hody towards the centre of ,he earth, is called the
fine
of
diu{li"" .
I n ¡his I¡ne all
he~vy
bodies deCcend,
if
oot
obllru!led_
Since the ",h oll! weight of a b'ody is united in its centre
of gravity, as thal centre aCcends or deCcends we mul1
Jook u'pon the whole bocly to do
Co
too..
Rut
as
it
is
contrary tO the "at']fe o f heavy bodit!s tOafcend of thei r
own
aecord, or
nOl
to
deCccnd wheo they are pernlitted;
we
maybe rure: th;tt, unlefs the centre of gr;.tvity be rup.
ported, ,he whole body \ViII ,umble or f.11. Hence i, is,
that (¡odies
Ch.ndupon (heir bares when the Ji"t: of d¡ree.
tion falls within lhe hafe; for i n this cafe the body can
not be m.&de tO fall without firl1 rai(jng the ('entre of gra–
vity higher lhan it
was
before. T hus, the incJining body
ASCO, (liR3 .)
wh~Ce
centre
oC
gnvity is E, (I, nds firm–
~y
on ilS baCe C D lK, becauCe ,he line of cjir<étion EF
f~lIs
\Vi,hin the baCe_ Hu, if a ",<iRh', as AllG H, be laid
1.1pnn (he tOr of the uod y. the c'!ntre of gravity of
th~
\1
hole body aud wcight ,ogc,hcr is raifcd up
10
1;
and
A
N
1
e
s,
35
and !hen, as the line of direétian ID falls without the·
u;.tfe at
D,
the centre of gravit)' I is OOl fupponed;
and·
lhe \IIhoJe bocly ao ...
1
wcight tumule down together .
The bro;¡der the baCe is, and lhe oe.Lrer the line of
d¡reélion is tO the middle o'r centre of il. the more.(irmly.
does the body llaod. On Ihe contrary, the narrower the
bafe, and lhe ne.Lrer Ibe Jine of direétion is
tO
the fide of
it . the mOre eafily m3y the body
b~
ovenhrown: a lef,
change of poCition being rufficient tO remove Ihe line o:
direétion out of the bafe io
lhe
Jan er cafe lhao
in
the
(armer. And hencc il
'SJ
that a fphere is fo eafily rolled'
upon a horiz.ontal plAne; and that il is fo difficult, if
no~
impoffibJe,
lO
make things which are lharp pointed to
Hand upright on the point.-From what hath beeo raid,
ir
plainly appears, that if rhe plaoe be inclined on which
the heavy body is placed, the body \ViII flide down upon
,he plane whiHl ,he line of direétion falls \V"hin the
b.Ce;
bU(
it
will tumble or roll down wheo that line faJls Wilh–
out the baCe_ Thus, ,he body A (6g_ 4.) will only flide
down the inclined plaoe CD, whilfl Ihe body B roll.
down upon it.
When the line of direétion fans within ,he baCe of our·
(eet, we fiand ; and mofi fi rmly,
WQ<'l
it is in the middle:–
bUl
",hen
it
is OUt of that bafe, we irnmedialely
fall.
Aod lt is nOI ooly pleaGng, but even Curprifiog, to (e–
fleét upon Ihe various and uothought o( melhods and po–
fiurc::s which we
~fe,
to retain this pofition, or tO recover·
il when
11
is Jol1. For this pnrpofe, we bend our uody
forward when we rife (rom a chair, or when we go up.
fiairs : and for Ihis purpofe aman leaos fonvard when he
carries
a
burden on h-is back, and backward
\IIhen
he car–
ríes it
00
his brean, aod tO the nghl or lefl fide as he–
carries
it
on the oppofile fideo
The
quantíty of matter in all bodi€s
is
in exaét
proportion lO their weights, bulk for bulk.. Therefore•.
heavy bodies are as much more den{e Or compaét than líght
bodies
oC
the Carne bulk, as theyexceed rhem in weight_
AII bodics are Cull of
~ore~,
or Cpaees void of maner :
.nd in gold, which is ,he heaviell of all known bodies,
there is perhaps a greater quarHity of {pace than of mat–
ter. For lhe particles of heal and magnelifm 6nd an
e~fy.
palf.ge,hrough the pores of gold; and even water i,C:lf
has beeo forcc.:d through Ihem. Befides, if we confider
ho\V eafily the
ray~
oflight p'Cs ,hrough
Co
Cohd a body as.
glafs, in alJ manDer
of
dire:étions,
\Ve
Chall
fiad
reafoD to
believe
thdt
bodies are exceedingly porous .
AII bodies are Come way or o,her affeétt d by hea, ;
and all metaJlic bodies ue expanded in lenglh , brea.dth,
and thicknefs Iheleby ,-The propon ion of the expan–
fion of feveral metals, according
10
th'e beH experiments,
i, nearly ,hus _ Iron .od glaC, as 3, neel 4, cúpper 4 and
one eighth, bra{s
S,
tin
6.
Jead
6
and one e:ighlh. An
iron rod
3
{eef long is about one 70th pan of an inch longer.
in fummer than in \ViOler.
The expaofioo
oC
me,al. by he." ·is demonllrated by
,he foll owing nta,hine, called a pyrome,cr.
AA
(fi g.
S.)
is a
fb,t picce of mahogony, io which art! fixcd (our brafs
llud!o
B,C,D,L;
and
lW·O
píos, one at F , and lhe othe"
at
H .
On the rin F lurns the: crooked ir.dcx El, and
upon lhe pin
H
,he
{l-r<!i~ht
indcx
GK;
;¡ga:nll which a
pieee of w.teh-Cprinc
R
bears gently, .nd
Co
prclres i,
towart..h