/It/ may happen that a colour does not alter, though placed at

different distances, when the thickness of the air and the distance

are in the same inverse proportion. It is proved thus: let A be the

eye, and H any colour whatever, placed at one degree of distance

from the eye, in a quality of air of four degrees of thickness; but

because the second degree above, A M N L, contains a thinner air by

one half, which air conveys this colour, it follows that this colour

will appear as if removed double the distance it was at before, viz.

at two degrees of distance, A F and F G, from the eye; and it will be

placed in G. If that is raised to the second degree of air A M N L, and

to the degree O M, P N, it will necessarily be placed at E, and will

be removed from the eye the whole length of the line A E, which will

be proved in this manner to be equal in thickness to the distance A G.

If in the same quality of air the distance A G interposed between the

eye and the colour occupies two degrees, and A E occupies two degrees

and a half, it is sufficient to preserve the colour G, when raised to

E, from any change, because the degree A C and the degree A F being

the same in thickness, are equal and alike, and the degree C D, though

equal in length to the degree F G, is not alike in point of thickness

of air; because half of it is situated in a degree of air of double the

thickness of the air above: this half degree of distance occupies as

much of the colour as one whole degree of the air above would, which

air above is twice as thin as the air below, with which it terminates;

so that by calculating the thickness of the air, and the distances,

you will find that the colours have changed places without undergoing

any alteration in their beauty. And we shall prove it thus: reckoning

first the thickness of air, the colour H is placed in four degrees of

thickness, the colour G in two degrees, and E at one degree. Now let

us see whether the distances are in an equal inverse proportion; the

colour E is at two degrees and a half of distance, G at two degrees,

and H at one degree. But as this distance has not an exact proportion

with the thickness of air, it is necessary to make a third calculation

in this manner: A C is perfectly like and equal to A F; the half

degree, C B, is like but not equal to A F, because it is only half a

degree in length, which is equal to a whole degree of the quality of

the air above; so that by this calculation we shall solve the question.

For A C is equal to two degrees of thickness of the air above, and the

half degree C B is equal to a whole degree of the same air above; and

one degree more is to be taken in, viz. B E, which makes the fourth.

A H has four degrees of thickness of air, A G also four, viz. A F two

in value, and F G also two, which taken together make four. A E has

also four, because A C contains two, and C D one, which is the half

of A C, and in the same quality of air; and there is a whole degree

above in the thin air, which all together make four. So that if A E is

not double the distance A G, nor four times the distance A H, it is

made equivalent by the half degree C B of thick air, which is equal

to a whole degree of thin air above. This proves the truth of the

proposition, that the colour H G E does not undergo any alteration by

these different distances.

/Chap. CCXCIX./--_Contrary Opinions in regard to Objects seen afar off._

/Many/ painters will represent the objects darker, in proportion as

they are removed from the eye; but this cannot be true, unless the

objects seen be white; as shall be examined in the next chapter.

/Chap. CCC./--_Of the Colour of Objects remote from the Eye._

/The/ air tinges objects with its own colour more or less in proportion

to the quantity of intervening air between it and the eye, so that a

dark object at the distance of two miles (or a density of air equal to

such distance), will be more tinged with its colour than if only one

mile distant.

It is said, that, in a landscape, trees of the same species appear

darker in the distance than near; this cannot be true, if they be of

equal size, and divided by equal spaces. But it will be so if the

first trees are scattered, and the light of the fields is seen through

and between them, while the others which are farther off, are thick

together, as is often the case near some river or other piece of water:

in this case no space of light fields can be perceived, but the trees

appear thick together, accumulating the shadow on each other. It also

happens, that as the shady parts of plants are much broader than the

light ones, the colour of the plants becoming darker by the multiplied

shadows, is preserved, and conveyed to the eye more strongly than that

of the other parts; these masses, therefore, will carry the strongest

parts of their colour to a greater distance.

/Chap. CCCI./--_Of the Colour of Mountains._

/The/ darker the mountain is in itself, the bluer it will appear at a

great distance. The highest part will be the darkest, as being more

woody; because woods cover a great many shrubs, and other plants,

which never receive any light. The wild plants of those woods are also

naturally of a darker hue than cultivated plants; for oak, beech, fir,

cypress, and pine trees are much darker than olive and other domestic

plants. Near the top of these mountains, where the air is thinner and

purer, the darkness of the woods will make it appear of a deeper azure,

than at the bottom, where the air is thicker. A plant will detach very

little from the ground it stands upon, if that ground be of a colour

something similar to its own; and, _vice versâ_, that part of any white

object which is nearest to a dark one, will appear the whitest, and

the less so as it is removed from it; and any dark object will appear

darker, the nearer it is to a white one; and less so, if removed from

it.

/Chap. CCCII./--_Why the Colour and Shape of Objects are lost in some

Situations apparently dark, though not so in Reality._

/There/ are some situations which, though light, appear dark, and in

which objects are deprived both of form and colour. This is caused by

the great light which pervades the intervening air; as is observable by

looking in through a window at some distance from the eye, when nothing

is seen but an uniform darkish shade; but if we enter the house, we

shall find that room to be full of light, and soon distinguish every

small object contained within that window. This difference of effect

is produced by the great brightness of the air, which contracts

considerably the pupil of the eye, and by so doing diminishes its

power. But in dark places the pupil is enlarged, and acquires as much

in strength, as it increases in size. This is proved in my second

proposition of perspective[73].

/Chap. CCCIII./--_Various Precepts in Painting._

/The/ termination and shape of the parts in general are very little

seen, either in great masses of light, or of shadows; but those which

are situated between the extremes of light and shade are the most

distinct.

Perspective, as far as it extends in regard to painting, is divided

into three principal parts; the first consists in the diminution of

size, according to distance; the second concerns the diminution of

colours in such objects; and the third treats of the diminution of the

perception altogether of those objects, and of the degree of precision

they ought to exhibit at various distances.

The azure of the sky is produced by a mixture composed of light and

darkness[74]; I say of light, because of the moist particles floating

in the air, which reflect the light. By darkness, I mean the pure air,

which has none of these extraneous particles to stop and reflect the

rays. Of this we see an example in the air interposed between the eye

and some dark mountains, rendered so by the shadows of an innumerable

quantity of trees; or else shaded on one side by the natural privation

of the rays of the sun; this air becomes azure, but not so on the side

of the mountain which is light, particularly when it is covered with

snow.

Among objects of equal darkness and equal distance, those will appear

darker that terminate upon a lighter ground, and _vice versâ_[75].

That object which is painted with the most white and the most black,

will shew greater relief than any other; for that reason I would

recommend to painters to colour and dress their figures with the

brightest and most lively colours; for if they are painted of a dull

or obscure colour, they will detach but little, and not be much seen,

when the picture is placed at some distance; because the colour of

every object is obscured in the shades; and if it be represented as

originally so all over, there will be but little difference between

the lights and the shades, while lively colours will shew a striking

difference.

AERIAL PERSPECTIVE.

/Chap. CCCIV./--_Aerial Perspective._

/There/ is another kind of perspective called aerial, because by the

difference of the air it is easy to determine the distance of different

objects, though seen on the same line; such, for instance, as buildings

behind a wall, and appearing all of the same height above it. If in

your picture you want to have one appear more distant than another, you

must first suppose the air somewhat thick, because, as we have said

before, in such a kind of air the objects seen at a great distance,

as mountains are, appear blueish like the air, by means of the great

quantity of air that interposes between the eye and such mountains.

You will then paint the first building behind that wall of its proper

colour; the next in point of distance, less distinct in the outline,

and participating, in a greater degree, of the blueish colour of the

air; another which you wish to send off as much farther, should be

painted as much bluer; and if you wish one of them to appear five times

farther removed beyond the wall, it must have five times more of the

azure. By this rule these buildings which appeared all of the same

size, and upon the same line, will be distinctly perceived to be of

different dimensions, and at different distances.

/Chap. CCCV./--_The Parts of the Smallest Objects will first disappear

in Painting._

/Of/ objects receding from the eye the smallest will be the first lost

to the sight; from which it follows, that the largest will be the last

to disappear. The painter, therefore, ought not to finish the parts of

those objects which are very far off, but follow the rule given in the

sixth book[76].

How many, in the representation of towns, and other objects remote

from the eye, express every part of the buildings in the same manner

as if they were very near. It is not so in nature, because there is no

sight so powerful as to perceive distinctly at any great distance the

precise form of parts or extremities of objects. The painter therefore

who pronounces the outlines, and the minute distinction of parts, as

several have done, will not give the representation of distant objects,

but by this error will make them appear exceedingly near. Again, the

angles of buildings in distant towns are not to be expressed (for they

cannot be seen), considering that angles are formed by the concurrence

of two lines into one point, and that a point has no parts; it is

therefore invisible.

/Chap. CCCVI./--_Small Figures ought not to be too much finished._

/Objects/ appear smaller than they really are when they are distant

from the eye, and because there is a great deal of air interposed,

which weakens the appearance of forms, and, by a natural consequence,

prevents our seeing distinctly the minute parts of such objects. It

behoves the painter therefore to touch those parts slightly, in an

unfinished manner; otherwise it would be against the effect of Nature,

whom he has chosen for his guide. For, as we said before, objects

appear small on account of their great distance from the eye; that

distance includes a great quantity of air, which, forming a dense body,

obstructs the light, and prevents our seeing the minute parts of the

objects.

/Chap. CCCVII./--_Why the Air is to appear whiter as it approaches

nearer to the Earth._

/As/ the air is thicker nearer the earth, and becomes thinner as it

rises, look, when the sun is in the east, towards the west, between the

north and south, and you will perceive that the thickest and lowest air

will receive more light from the sun than the thinner air, because its

beams meet with more resistance.

If the sky terminate low, at the end of a plain, that part of it

nearest to the horizon, being seen only through the thick air, will

alter and break its natural colour, and will appear whiter than over

your head, where the visual ray does not pass through so much of that

gross air, corrupted by earthy vapours. But if you turn towards the

east, the air will be darker the nearer it approaches the earth; for

the air being thicker, does not admit the light of the sun to pass so

freely.

/Chap. CCCVIII./--_How to paint the distant Part of a Landscape._

/It/ is evident that the air is in some parts thicker and grosser than

in others, particularly that nearest to the earth; and as it rises

higher, it becomes thinner and more transparent. The objects which

are high and large, from which you are at some distance, will be less

apparent in the lower parts; because the visual ray which perceives

them, passes through a long space of dense air; and it is easy to prove

that the upper parts are seen by a line, which, though on the side of

the eye it originates in a thick air, nevertheless, as it ascends to

the highest summit of its object, terminates in an air much thinner

than that of the lower parts; and for that reason the more that line

or visual ray advances from the eye, it becomes, in its progress

from one point to another, thinner and thinner, passing from a pure

air into another which is purer; so that a painter who has mountains

to represent in a landscape, ought to observe, that from one hill

to another, the tops will appear always clearer than the bases. In

proportion as the distance from one to another is greater, the top will

be clearer; and the higher they are, the more they will shew their

variety of form and colour.

/Chap. CCCIX./--_Of precise and confused Objects._

/The/ parts that are near in the fore-ground should be finished in a

bold determined manner; but those in the distance must be unfinished,

and confused in their outlines.

/Chap. CCCX./--_Of distant Objects._

/That/ part of any object which is nearest to the luminary from which

it receives the light, will be the lightest.

The representation of an object in every degree of distance, loses

degrees of its strength; that is, in proportion as the object is more

remote from the eye it will be less perceivable through the air in its

representation.

/Chap. CCCXI./--_Of Buildings seen in a thick Air._

[Illustration]

/That/ part of a building seen through a thick air, will appear less

distinct than another part seen through a thinner air. Therefore the

eye, N, looking at the tower A D, will see it more confusedly in the

lower degrees, but at the same time lighter; and as it ascends to the

other degrees it will appear more distinct, but somewhat darker.

/Chap. CCCXII./--_Of Towns and other Objects seen through a thick Air._

[Illustration]

/Buildings/ or towns seen through a fog, or the air made thick by

smoke or other vapours, will appear less distinct the lower they

are; and, _vice versâ_, they will be sharper and more visible in

proportion as they are higher. We have said, in Chapter cccxxi. that

the air is thicker the lower it is, and thinner as it is higher. It is

demonstrated also by the cut, where the tower, A F, is seen by the eye

N, in a thick air, from B to F, which is divided into four degrees,

growing thicker as they are nearer the bottom. The less the quantity of

air interposed between the eye and its object is, the less also will

the colour of the object participate of the colour of that air. It

follows, that the greater the quantity of the air interposed between

the eye and the object seen, is, the more this object will participate

of the colour of the air. It is demonstrated thus: N being the eye

looking at the five parts of the tower A F, viz. A B C D E, I say,

that if the air were of the same thickness, there would be the same

proportion between the colour of the air at the bottom of the tower and

the colour of the air that the same tower has at the place B, as there

is in length between the line M and F. As, however, we have supposed

that the air is not of equal thickness, but, on the contrary, thicker

as it is lower, it follows, that the proportion by which the air tinges

the different elevations of the tower B C F, exceeds the proportion

of the lines; because the line M F, besides its being longer than the

line S B, passes by unequal degrees through a quality of air which is

unequal in thickness.

/Chap. CCCXIII./--_Of the inferior Extremities of distant Objects._

/The/ inferior or lower extremities of distant objects are not so

apparent as the upper extremities. This is observable in mountains

and hills, the tops of which detach from the sides of other mountains

behind. We see the tops of these more determined and distinctly than

their bases; because the upper extremities are darker, being less

encompassed by thick air, which always remains in the lower regions,

and makes them appear dim and confused. It is the same with trees,

buildings, and other objects high up. From this effect it often happens

that a high tower, seen at a great distance, will appear broad at top,

and narrow at bottom; because the thin air towards the top does not

prevent the angles on the sides and other different parts of the tower

from being seen, as the thick air does at bottom. This is demonstrated

by the seventh proposition[77], which says, that the thick air

interposed between the eye and the sun, is lighter below than above,

and where the air is whiteish, it confuses the dark objects more than if

such air were blueish or thinner, as it is higher up. The battlements

of a fortress have the spaces between equal to the breadth of the

battlement, and yet the space will appear wider; at a great distance

the battlements will appear very much diminished, and being removed

still farther, will disappear entirely, and the fort shew only the

straight wall, as if there were no battlements.

/Chap. CCCXIV./--_Which Parts of Objects disappear first by being

removed farther from the Eye, and which preserve their Appearance._

/The/ smallest parts are those which, by being removed, lose their

appearance first; this may be observed in the gloss upon spherical

bodies, or columns, and the slender parts of animals; as in a stag,

the first sight of which does not discover its legs and horns so soon

as its body, which, being broader, will be perceived from a greater

distance. But the parts which disappear the very first, are the lines

which describe the members, and terminate the surface and shape of

bodies.

/Chap. CCCXV./--_Why Objects are less distinguished in proportion as

they are farther removed from the Eye._

/This/ happens because the smallest parts are lost first; the second,

in point of size, are also lost at a somewhat greater distance, and so

on successively; the parts by degrees melting away, the perception of

the object is diminished; and at last all the parts, and the whole, are

entirely lost to the sight[78]. Colours also disappear on account of

the density of the air interposed between the eye and the object.

/Chap. CCCXVI./--_Why Faces appear dark at a Distance._

/It/ is evident that the similitude of all objects placed before us,

large as well as small, is perceptible to our senses through the iris

of the eye. If through so small an entrance the immensity of the sky

and of the earth is admitted, the faces of men (which are scarcely any

thing in comparison of such large objects), being still diminished by

the distance, will occupy so little of the eye, that they become almost

imperceptible. Besides, having to pass through a dark medium from the

surface to the _Retina_ in the inside, where the impression is made,

the colour of faces (not being very strong, and rendered still more

obscure by the darkness of the tube) when arrived at the focus appears

dark. No other reason can be given on that point, except that the speck

in the middle of the apple of the eye is black, and, being full of a

transparent fluid like air, performs the same office as a hole in a

board, which on looking into it appears black; and that those things

which are seen through both a light and dark air, become confused and

obscure.

/Chap. CCCXVII./--_Of Towns and other Buildings seen through a Fog in

the Morning or Evening._

/Buildings/ seen afar off in the morning or in the evening, when there

is a fog, or thick air, shew only those parts distinctly which are

enlightened by the sun towards the horizon; and the parts of those

buildings which are not turned towards the sun remain confused and

almost of the colour of the fog.

/Chap. CCCXVIII./--_Of the Height of Buildings seen in a Fog._

/Of/ a building near the eye the top parts will appear more confused

than the bottom, because there is more fog between the eye and the top

than at the base. And a square tower, seen at a great distance through

a fog, will appear narrower at the base than at the summit. This is

accounted for in Chapter cccxiii. which says, that the fog will appear

whiter and thicker as it approaches the ground; and as it is said

before[79], that a dark object will appear smaller in proportion as it

is placed on a whiter ground. Therefore the fog being whiter at bottom

than at top, it follows that the tower (being darkish) will appear

narrower at the base than at the summit.

/Chap. CCCXIX./--_Why Objects which are high, appear darker at a

Distance than those which are low, though the Fog be uniform, and of

equal Thickness._

/Amongst/ objects situated in a fog, thick air, vapour, smoke, or at

a distance, the highest will be the most distinctly seen: and amongst

objects equal in height, that placed in the darkest fog, will be most

confused and dark. As it happens to the eye H, looking at A B C, three

towers of equal height; it sees the top C as low as R, in two degrees

of thickness; and the top B, in one degree only; therefore the top C

will appear darker than the top of the tower B.

[Illustration]

/Chap. CCCXX./--_Of Objects seen in a Fog._

/Objects/ seen through a fog will appear larger than they are in

reality, because the aerial perspective does not agree with the linear,

viz. the colour does not agree with the magnitude of the object[80];

such a fog being similar to the thickness of air interposed between the

eye and the horizon in fine weather. But in this case the fog is near

the eye, and though the object be also near, it makes it appear as if

it were as far off as the horizon; where a great tower would appear no

bigger than a man placed near the eye.

/Chap. CCCXXI./--_Of those Objects which the Eyes perceive through a

Mist or thick Air._

/The/ nearer the air is to water, or to the ground, the thicker it

becomes. It is proved by the nineteenth proposition of the second

book[81], that bodies rise in proportion to their weight; and it

follows, that a light body will rise higher than another which is heavy.

/Chap. CCCXXII./--_Miscellaneous Observations._

/Of/ different objects equal in magnitude, form, shade, and distance

from the eye, those will appear the smaller that are placed on the

lighter ground. This is exemplified by observing the sun when seen

behind a tree without leaves; all the ramifications seen against that

great light are so diminished that they remain almost invisible. The

same may be observed of a pole placed between the sun and the eye.

Parallel bodies placed upright, and seen through a fog, will

appear larger at top than at bottom. This is proved by the ninth

proposition[82], which says, that a fog, or thick air, penetrated by

the rays of the sun, will appear whiter the lower they are.

Things seen afar off will appear out of proportion, because the parts

which are the lightest will send their image with stronger rays than

the parts which are darkest. I have seen a woman dressed in black,

with a white veil over her head, which appeared twice as large as her

shoulders covered with black.

MISCELLANEOUS OBSERVATIONS.

LANDSCAPE.

/Chap. CCCXXIII./--_Of Objects seen at a Distance._

/Any/ dark object will appear lighter when removed to some distance

from the eye. It follows, by the contrary reason, that a dark object

will appear still darker when brought nearer to the eye. Therefore the

inferior parts of any object whatever, placed in thick air, will appear

farther from the eye at the bottom than at the top; for that reason the

lower parts of a mountain appear farther off than its top, which is in

reality the farthest.

/Chap. CCCXXIV./--_Of a Town seen through a thick Air._

/The/ eye which, looking downwards, sees a town immersed in very thick

air, will perceive the top of the buildings darker, but more distinct

than the bottom. The tops detach against a light ground, because they

are seen against the low and thick air which is beyond them. This is a

consequence of what has been explained in the preceding chapter.

/Chap. CCCXXV./--_How to draw a Landscape._

/Contrive/ that the trees in your landscape be half in shadow and half

in the light. It is better to represent them as when the sun is veiled

with thin clouds, because in that case the trees receive a general

light from the sky, and are darkest in those parts which are nearest to

the earth.

/Chap. CCCXXVI./--_Of the Green of the Country._

/Of/ the greens seen in the country, that of trees and other plants

will appear darker than that of fields and meadows, though they may

happen to be of the same quality.

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