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o

T

a"d therefore. when the

run

is

al

l.

below Ihe horizon

H,

thole rays whieh go

00

in the free fpace

lkK

pref<rve a

r,eéliJir.e.,J eourfe until they f. 1I upon the tOP of the ato

morpbere ; amI tbofe wbicb fall fo about

K.

are refraéld

at their entrance ioto fhe

atmofphere,

and beot down in

the line

¡(mB,

tO

the obfern."r's pJace

al

B :

;:¡nd there·

fare, to him tbe fuo ",ill appear at

L,

in the dirc,'!ioo of

the

(ay

B~nK,

above tbe horizon

BCH,

'wheo he is real!y

beJow it at

l .

The angle eontained between a ny of light, and a pero

pendicular to the refraéling furfaee, is ealled

Ih! ansl,

of

inci:lence.'

and che aogle coctained betwecn

lhe

(ame per–

pendicular, and the fame " y after refraéhon, is e.lled

,he

angle

ofrifraflion.

Thu. (No. 4.) let

LBfIil

be the

refraélin~

fu rfaee of a mediom (ruppofe water,) and

ABr:

a perpendicular tO that furfaee; let

J)

B

be a ray of light,

goi·ng <?ut of air loto water at

B

J

and thercin refraéted in

t·he line

BH;

tbe angle

ABD,

is th.e angle of ineideoee,

of whieh

DF

is the fine; aDd the angle

KBH

is the an–

gle of.refraélioo, 'waofe fin e is

KI.

Vvhen the refraéling mediuOl is water, Ihe fine of the

angle of ineidence is tOtbe fine of the angle of rdraélion

as 4 tO 3; whieh is eonfirmed by tbe following experi.

ruent, uken from Ooélor

SMITH '~

Optles .

D eferihe tbe eirele

DAEC

on aplane fquare board,

2nd

eroC,

it at ,i¡ht angles witb tbe !lraigbt liDes

ABC,

and

LBfIil;

then, from the interfeélion

A,

with aoy

0-

peniDg of the compalfes. fel off the eq'13\ ares

AD

and

AE,

and draw the right lioe

DFE:

then, takiog

Fa,

whieh i. three quarters of the leogth

FE,

from the poiot

IZ,

draw

al

parallel to.

ABK,

and join

KI

parallel to

BM:

fo

K!

\ViII be equal to three quarters of

FE

or of

DF.

This dooe;

6"

the board uprjght upoo the leadeo

peddhl

O,

and !lick tbree pios perpendieularly into the

board,

at

the points

D, B,

and

1:

then fet the board

upright into th.e velfel

T UV.

aod 611 up the velTeI with

water

to

the line

LB/lf.

When the water ba, fettled,

¡ook along the lioe

DB,

fo as you may fee the head of

the pin

B

over the head of the pio

D ;

and the pin

1

,viII appe" in the fame right line produeed to G, for i..

he.d will be feeo ju!l over the head of the pin at

B :

whieb file"'s tbat the ray

lB,

eomiog from the pin at

1,

is fo refnéted at

B)

as to proceed from theoce

in

the

line

BD

to the eye oftheobferver

¡

the 'ame as it would

do from any point

e

in the right line

DBC,

if there

were no water in the vefTd:

and airo

Ihews, (hat

KI,

the fine of

rerraélioD

in water, is to

DF,

tbe fine of io.

.cidence io air, as 3 to 4.

Henee, if

DBH

were a erooked fliek put obliquely

ioto (he water,

il

would appear a (haight one

al

DOG.

Therefore, as the line

B

H

appears at

BC,

Co~he

line

BC

will appear at

Bg;

and eonCequeotly, a flraight !liek

DBC

put oblrquely into water, will feem beot at tbe furface

of the water io

B,

aod erooked, as

DBg.

Wheo a ray of light palTes out of air ioto glaCs, the

(ine of

incidence

is to the fine of

n:fraétion

as 3 to

2 ;

and when

OUt

of air ioto a diamood, as 5 to

2.

OfGLASSES.

GL ASS may be grouod into eight diffcreot Chapes at

lean, for optiea) purpofe.,

"iz.

e

s.

.. A

plan,

glaft,

(No. 5.) whioh is Bal on both fid..,

and .of eqttal thicknefs in all pans, as

A.

2.

A

pltJnc-com.,'ex,

\fJhich is ilat

00

one lide. and con·

vex on lhe other, as

B.

3. A

d,)U{¡Ü-.&'fiV~X,

wbkh

is convex on

both fides,

as

C.

4. A

plano-concQtle,

which is fIat on one fid e, and

conca've on the other, as

D.

S.

A

doubl, ronca"e,

whieh is eoneave

00

both fide.,

as

E.

6.

AJIUnifouI,

which is coocave

00

one Cide, and

convex..

on [he

other, -as

F.

7. A

Jln'

plano'

con",,,,

·whofe eonvex fide is ground

into Ceveral liule Rat furfaees, as

e.

8. A

priJiJJ,

whieh has three

flat

fides; and when

viewed endwife, appears like an equilateral triaogle, as

H.

GlalTe••ground ioto any. of the Ibapes

B, C, D, E, F,

are gener.lly ealled

lenfu.

A right lioe

L/K,

.(ND. 6.) going pe'pendieularly

througb the rniddle of a leos, is calle<!

Ih, axil

of

,he

lent .

A ray 'of light

Ch,

falliog perpendieularly on aplane

glaC.

EF,

will.pafs through the glafs in the rame diree–

tion

hi,

and go

out of

it ioto the air in the [ame right

courfe

iH.

A ray of light

AB,

f.lling obliquely

00

a plaoe glafs.

will go out of tbe glafs in the

fa.le

direélioo, but not io

the Came right Iioe: for in touehing the glaf" it will

be r<fraéted in the I:ne

BC;

and in leaving the glaC" it

will be reFraéled io the line

CD.

A ray'

~f

light

CD,

(No. 7.) falling obliqucly on the

middle of a eonvex glafs, will go forward io tbe

f.me

direélion

DE,

as if it had fallen with the fa me degree of

obliquity

00

aplane glafs; aod will go out of the glaC.

in

lhe fame

direétion with which it

entered

: for it will

be <quallr refr.é1ed at the points

D

and

E,

as if it had

p.rred through aplane fudace . But the rays

ce

and

el

will be fo reFnéled, as to meet agaio at the poiot

F.

Therefore, .11 the ráys wnieh Row from the point

C

r

fo as to go th,ough the glaCs, will meet again at

F;

aod

if they go farthe r onward , as to

L,

.hey erofs

al

F,

aod

go forwá rd

00

the oppofite lides of the middle ray

CDEF,

to what they ",ere in approaehing it io the direélioo.

HF

and

KF.

When paralle! ray', as

A

BC,

(No. 8.) fall direélly

upon a plano.eoovex glaCs

DE,

and pafs through it, they

will be fo refroéled, as tO unite io a point.f behiod it

¡

aod this poiOl is ealled the

principalfoClu;

the di nance of

whieh, from the middle of the glafs, is ealled the

f ocal

diJIan« ,

whieh is equal to twice the radius of the fphere

of the glafs's convexity. And,

When parallel rays, as

.1BC,

(No. 9.) fall direélly

upon a glaf.

DE,

whieh is equally eonvex

00

both fides,

and pafs through it ; they will be fa refraéled, a.

10

meel

in a point o, principal foeus

¡;

whofe diflanee is equal to

the radius or femidiameter of the fphere of the glaf,',

convexity. But if a glaf. be more eoovex

00

one fide

th.n

00

the other. the. rule for fioding the focal dillanee

is tlris: As the fu·m of the fernidiameters of both eon–

vexities is

10

the remidiameter of eitbel, fo is double the

fem idiameter