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o

p

T

rallc1 10 Ihe eye afler p.lling Ihrough Ihe glaC. ; and Ibeo,

b)' <Iltering Ihe eye al

e.

h<y will be converged 10 .s

013ny

difFerent

pOlOts on

the

retina,

a~d

form a

large

in–

venc:d pillure

AD

UpOD

¡t,

as

in

the figure.

To 6nd how mueh Ibis

gl.Cs

magniGes, Ji.ide Ihe le.O:

dinance (whieh is abou, Gx inehes)

al

whieh an objeél

can b. Ceen diOinélly \Vilh Ihe bare eye,

I

y me foe.1 dif–

Unce of ,he glaCs; and Ihe '1uolienl will fhe\V how mueh

Ihe glafs magnifies Ihe diame,er of ,he objeél.

The

do.hlt

or

compoul1d miero(cop.,

(No. 18.) confiO.

of an

objeél-gl.Cs

<d,

and an eye-glaf••

¡:

-The. fmall

objeél

"b

is placed

al

a Iiltle crealer diOance from Ihe

glaC.

cd

Ihan i" principal foeus , fo Ih.. Ihe peneils of ray'

1I0wing from Ihe diiferenl poin.. of Ihe objeél, and paf•.

ing II,"rough Ihe

gl.fs

, may be

m.de

10 converge and u·

nife in as many points

bctu'eeng

and

h,

where the image

of Ihe objeél \ViII be formed : .whieh image is viewed by

,he eye threufh 'the eye-glafs

if.

For the eye.glafs be·

ing

Co

plaeed , Ih.. the image

gh

may be in ils focus. and

'he eye mueh about the Came diOanee on .he olber fide,

the rays of eaeb peocil will be paralle!, afler , oing out

of Ihé eye.glaC., as

al •

and

r.

liU ,hey come 10 Ihe eye

.1

1,

where, they \ViII begin 10 converge by lhe refraélive

power of lhe bumours; and after having crolred eaeh o –

t~er

in the pupil, and palTed through lhe ehry'lalline

a.l d "itreaus humours, they will be colJeéled iota

poin

.s

00

lhe

relÍo3,

and (orm ,he

large

¡overted

image

AD

lhereoo.

Tbe ,matnifying power of Ihis mierofeope is as follo·Ns.

Suppofe lhe image

gh

to be fix times lhe dinance of lhe

objeél

ab

from Ihe

obj.él

-flaC.

ed;

then \ViII Ihe image

be fix limes the lenglh of the objeél: but finee ,he image

eould nOl be feen dillinll ly by lhe bare eye al a lefs dif–

tance lhan fix inehe. , if it be -"iewed by an eye-glafs

if,

of one ioeh foeu.,

¡¡

will thereby be brought Gx limes

noarer the

ere;

and coofcquendy vicwed under an angle

lix times as large

~5 ~efore

;

fo thu

jt

will be agaío mag–

ni6ed Gx limes; that is. fix limes by the objetl-glafs,

and fix times by the eye-glaf.; whieh multiplied in,o one

another, m"kes 36 times; and (o much

i5

lhe objeét mag–

nified in diamettr more than what

ir

appears t6 lhe bare

eye ; and eoofequeDtly 36 time. 36, or 1296 times, in

furface.

But, beeaufe lhe extent or field of

,'i.\V

is very fmaU

in this mierofeope, there are generally tWO eye-glalles

placed rgmetimes clore .logether, and fomctimes

3n

¡oeh

.funde<; by wliieh ,means, although lhe ohjcél app.a"

lefs

m~gni6ed,

yet 'lhe vilible area is nlueh enlarged by

Ihe iDterpof"ion of, feeond eye 'e lac" and conCequently

a mnch plearanter view

¡,

obtained.

The

fo/ar ",ierofeop.,

(No. 19. ) invenled l>y Dr L ie–

berkhun,

j.

eooOruéled in lhe f9Uowing manger, H ..ing

procu rcd a very dark room, let a rouod hole be madc in

the window· OlUuer, aboul three ¡oches diameter, through

\I'hieh th. fun m. y

e.tl

a 'ylinder of

r.ys

AA

ioto the

room . In

lhis

hoJe, pl:tce

Ihe

cnd of a tube, containing

t\Vo

.eonvex glalTe. and an cbjcél,

"iz.

l .

A eonvex glaC.

n.o

of ahola t\Va

incl1f~5

diameter, and three ¡ochcs

focal

dillance, is to be pldced in that fntl of che 11lbc which is

pUl into lhe hol..

2 .

The objeél

bb,

l>einc

pUl

be,

w.en

t wo glalfe. (which muft be eODeave 10 hold il al ¡il>crty)

e

s.

421

is plaeed abou t two inehes and a half from th. &1,Cs

aa.

3, A

liule more Ihan a quarter of an ineh from Ibe objeét

i. plaeed Ihe fmaU eor.vex glar.

ce,

whofe focal diOanee

is a quarttr'" of ao ancho

The lube may be fo plaeed, when the fun is low, that

his rayo

AA

may en'er direélly inlO it: but when he i.

high , his rays

nn

muO be refieéled inlo

tb~

tube by lhe

plane mirroar or looking gl.f.

ce.

Tllings being thu. prepared, lhe ra)'s Ihat enter th

tuhe \ViU be eonveyed by the glaC.

(la

10IVarcls rhe objeél

¿b,

by whieh means it wiU be Orongly iUuminated ; and

the rayo

d

whieh flo\V from ir lhrough lhe eonvex glaf.

u,

wiU make a large inverted piélure of the objeél .1

D D,

whi ch. being recelved on

a

whitc paper,

wiJl

repr:fcht

the objeél 0I.gni6ed io len¡¡lh, in proponinn of Ihe dif–

tanee of the piélure from the glaf.

u ,

to lhe diOance of

the obj. él from ,he fa me glafs . T hus, fuppoCe the

diC–

tanee of Ihe objeél from the

gl.Cs

10 be .;.. por" of an

ineh, and the d;naoee of the dillinél piélqre 10 be 12

ft:et

or

144

inches, in

which

(here are

1440

tenth, of

ao

¡neh; and this number dividcd by

3

tenth!, g'ives

480 ;

which

is

the numbcr

o(

times the piélure

is

longer or

broad.. Ihan the objeél; and the length multiplied by

the br.adlh, OleIVs how mueh the \Vhole furface is ml&.–

niGed.

Of

TEL<s coPE'.

B

E

ro

R E

\\le

enter upon the defcriptioD of tclcrcores,.

it \ViU be proper tO fhew bow lhe rayo of light are affoc–

ted by palling lhrough concave glalfes, ¡od al Co by faJlin¡

upon concave mirrnun.

~

When paralleJ ray', as

(lbcdifgh.

(No.

20,)

pafs di·

reélly thr9ugh a gl.C.

AB,

which il . equaJly

eone.ve

oe

both Gde., they will diverge after palling Ihrough Ihe glaCs,

as if they had come from

a

radiant poinr

e,

~

the centre.

of lhe glafs's concavity; which poinr is caJJed the

riega".

lave or virtual focus of Ihe glafs. Thu\ the

ray

n,

afte;

p.lling Ihrougb lhe glaCs

AB,

\ViII &oon in th. direétioD

Al,

a. if it had proceeded from he POiOI

e,

aod no gl.C.

been io Ihe \Vay. Tbe ray

b

wiU )lo on in Ihe

di re~lioo

nlll;

the

ray

e

in

the direélion

gp.

&c.-The ray e , th;.t

fall. dir.élly upon the middle o'f the glaCs, (ufft " DO

refraél ion in pafling lhrough il;

hUI

goes on

in

th~

fame

rell iline.1 direélion, as

i,f

no glaC. had been in itS way.

I(

lhe glaf. had been eoneave only on one fide, :md lhe

olher fide quite pl. ne, Ihe

r.ys

wnuld have diverted. af–

ler palling lhrough, il, as if lhey had come froOl" radian,

poinl al dQuble lhe diOanee of

e

froOl

th~

gbfs; Ihat is ,

as if the radiant had bern . t ,he d,lI.nce o( • \Vhole di.:

meter of the glafs', conca\'ity.

lf

rays come more eonverging to Cueh a glafs, than P"

rallel ray$ diverge after pat1ing Ihrough il. Ihey \ViII eon–

tinue to converge after p:;l1ing

t)l¡,ough

it;

OUt

will

nct

mee' Co foon as if no glaCs had beeo in the

w.)',

aud will

incline tOward..

l

the fame lide ro which they would h;:!.vc

divereed ir they had come pa ralld 10 Ihe gl.l5. Thus

Ihe rays filnd

h,

going in a converg:ngflate lowards che

cdge of the

n1ars

al

B,

and converging

mor~

in th eir

w;y

to it than lhe paralld rays

diver~e

.fter Falling lhrough

it, lhey will go on

eonv~rsin&

af,er they r afs t1:rouch

ir,

thou~'l