o
p
T
c..ity. the image and ohjea IVill be coiocideot, and equa!
in bulk.
1f
aman pl.ces himlelf
dire~ly
before a large concave
mirrour.
bUl
fanher
fro{II
it
thao its
centre
ol"
conc:\VilY,
be
wilJ
fee an ¡overteú image of himfelf in the air, be–
twecn him :lnd tbe mirrour, of a Jefs (ize than
himrclf.
Ana if he holds out his hand IOwanls the mirrour, the
hand of
lhe
image \ViII come
OUt
towards his hand, and
coincide with ir, of an equal bulk, when his }¡,tnd is in
the centre of
conclvity
j
al\d he \ViII imagine he mayfllake
hands with his image. If he reaches his hasd
hrther,
the haod of the im. ge IViil pafs by his haod, and come
between his hond and his body: and if he moves his
hand towards either Jide, the hand of the image will
move towards th1! other; fo that whatever way [he ob–
jea moves, the
imagé..will
move the
contrary.
AII the ",hile a by:n;nder will fee nothing of the i–
mage, becaufe nooe of tbe reBeaed rays that form it enter
bis eyes.
If
a fire he made io
a
large room, and a fmooth ma–
hogony table be placed at a good dinance near the IVall,
before
a
large concave mirrour; fo pl.ced, tbat the light
of ihe fire may be refleaed from the mirrour to its focus
upon the table; if
t
perfon f1ands by the table, he will
fee nothing upoo it but a 10ngiO. beam of light: but if
he (lands at a dinance towards the Gre, not direaly be–
tweeo [he fire and rríirrour, he will Cee an image of the
6fe
upon the table, large .od erea. And if another perfon,
who koows nothing of this ma"er before-hand, fhould
chanee to come into ,he room, and fltOuld look from the Gre
to\Vards the table, he would be nartled at the appearaoce;
for the table would feem to be on lire, and, by being near
the waiofcot, 'o endanger ,he who!e houfe. In this e"–
perimeot, ,here fhould be no light in the room buí wha,
proeeeds from th. lire; and the mirrour ought to be at
lean fifteen inches in Eliameter.
lf
the lire be darkened by • fcreen , and a large candle
be placed at ,he back of the fcreen; a perfon f1anding by
the c.ndle will fee tbe 'ppearaoce of a fine large n ar, or
.ather planet, upon the .áble, as bright as Venus or Jupi–
ter. And if a fmal! \Vax taper (whofe llame is much lefs
than .he llame of .he candle) be placed near .he candle, a
latellite to the planet will appear
00
the table : and if the
taper be moved rouod the candle, the fatellite wiU go
round the planet.
In a
r'írofling ¡'/'!c"P',
the glafs \Vhich is nearen the
?b jetl in viewing i, is called the
objrfl-g/oft,
and that which
IS
nearen the eye i. called
¡he 'Je-g/oft.
The obje{t–
glafs mun be convex, bU! the eye_glafs may be either coo_
vex or concave: and generalIy, in lookiog through a te·
I.fcope, the eye is in the focus of the eye-glafs; though
that is not very material: for [he
dictance
of the eye, as
to difiinét vHion, is jndifFerent, providcd the ray! of [he
peocils fall upoo it parallel: only, the ncarer the eye is
to the end uf the «Iefcope, the larger is th< fcope or area
of the field of view,
L et
cd
(No_
23 )
be a convex glaf. G"ed in a long tube,
2nd bave its focus at
E .
Then, a peneil of rays
gh;,
.8Q
w
ing from the upper extremity
A
of the remote objea
AD,
will be fo refraéled
1y
palling through the gl. fs, as
to
conver~e
and nleet in the poiotí; whilfl the pencil of
r.ly'
Um,
1I0wing from the 10\Ver extr<mity
H
of the
VO l.. lII. N° . 87.
z
1
e
s-
fame objeél
An,
aod paliing through the
gl.fs,wiU coo–
verge and mece
iD
the point
e:
and the images of the
poiots
A
and
B
\Vil! be formed in the pointS í"nd , _ And
as all [he intc.:rmediate points . of lh'e objeEt, belween
A
and
D,
{cnd out pencils of rays in the fame manner, a fuf·
licient n"mber ofthefe pencils wil! pars through the ob–
jeél:,glars
c.t,
and
converge
lo
as many
intermedlítte points
between
e
andí; and fo wil! form 'the whole ioverted i–
mage
eEí
of the dinina objea. But
b~caufe
this imag.
is fmall. a concave glafs
no
is fo placed in the end of the
lube neXl
the
eye, lhal
ilS
virtual
focus
may be al.
F.
And as the pencils of rayo pafs eonverging through the
coneave glafs, but converge lefs after palling through it
than befare, they go on
further,
as
tO
b
and
a ,
before
lhey
meet; and the pencils them(cl ves being made
to
diverge by polling through the
cunc.veglafs. they enter
the eye, and form the large piéture
ah
UpOD
the retioa,
whereon it is
magnifiad
uoder the
aDgle
bFao,
BUl
this telcfcope
has
ene inconveniency which. reoders
it unfit for mon purpofes, which is, th.t .he pencil, of
rays being made to diverge by
pailin~
through the con–
c.veglafs
no,
very few of them caD enter the pupil of the
eye; and therefore the lield of view i. but very fm.I!,
as is evident by the figure. For DODe of the peocil.
which
Bow
either from the tOP or boltom ofthe objea
AH
can enter the pupil of the eye at
C,
bu' are al! f10pt by
fal!ing upon the iris above aod below the pupil : .nd there–
fore, ooly .he nliddle par< of theobjea can be feeo when
the telefcope lie-, direaly ,oward. it, by means of thofe
rays which proce¿d from the middle of the objea.
S"
that
to
fee the whole of it, the telefcope muC! be moved
upwards aud dOWOW'fd., unlef. the objea be very re–
mote ; and then it is oever feen dinioélly.
This
inconvenience
is
remedied
hy
(ubflituting
a con–
vex eye-glafs. as
gh,
(No.
24')
in place of the eoneave
one; and fixing
ir
fo in lhe lube, lhat its foc us may
be coincident with the focus of the objea-glafs
cd,
as
at
E.
For theo, the rays of the peneils 1I0wing
from the objea
AH,
and paffing through the objea-glafs
cd,
will meel in its focus, and form the ioverted
i–
mage
mEp:
and as .he image .is forOled in the focus
of the eye-glafs
gh,
the
ra.ysof each peneil will be pa–
rallel, after palling ,hrough that glafs; but the pencil.
themCe1ves will croCs in ¡ts focus
00
the other
fide,
as al
e :
aod the pupil of the eye beiog in thi. focus, the_i–
mage \Vill be vie\Ved througb the glafs, under the angle
geh
;-
and being at
E,
it wil! appear magni6ed, fo as tO
lil! the whole fpace
CmepD.
But,
as this
teleCcope
inTerts
the image
Wilh
refpett
to
lhe objeét,
jI
gives an
unpleafant
view cf terrdlrill
objeas; and is ooly fit for viewillg tbe henenly bo–
dies,
in
which we
regard
not'their pofitioo, becaufe their
being ¡nverted
does
not
appeu
on
aCCQunt
oE
their being
round.
But
wh:uever way the objeét íeems
tO
move.
[his
teJeCcope
mull be
moved
che
contrar}"
wt\~-r)
in
crder
to keep
fight
of it
j
(o r, fince the ebjeét is ¡overted,
i11
motion will be fo
too .
The m.gnif)'ing power of this telefcope is 's <.he focal
dinance of the objeét-glafs to the focal
diO.nc< of the
eye-gl.fs.Therefore. if the former be divid<d -b)' the
l,oltter,
the
quoticnt
will
expre(s che m2gnifying powcr.
V/hen \Ve fpeak of the magnifying of a tel<fcope or micro-
5
O
t
fco!,e,