5. THE LAW OF RADIATION.

210. We have hitherto been concerned only with the binding of our

various objects into beautiful lines or processions. The next point we

have to consider is, how we may unite these lines or processions

themselves, so as to make groups of _them_.

[Illustration: FIG. 41.]

[Illustration: FIG. 42.]

Now, there are two kinds of harmonies of lines. One in which, moving

more or less side by side, they variously, but evidently with consent,

retire from or approach each other, intersect or oppose each other;

currents of melody in music, for different voices, thus approach and

cross, fall and rise, in harmony; so the waves of the sea, as they

approach the shore, flow into one another or cross, but with a great

unity through all; and so various lines of composition often flow

harmoniously through and across each other in a picture. But the most

simple and perfect connection of lines is by radiation; that is, by

their all springing from one point, or closing towards it; and this

harmony is often, in Nature almost always, united with the other; as the

boughs of trees, though they intersect and play amongst each other

irregularly, indicate by their general tendency their origin from one

root. An essential part of the beauty of all vegetable form is in this

radiation; it is seen most simply in a single flower or leaf, as in a

convolvulus bell, or chestnut leaf; but more beautifully in the

complicated arrangements of the large boughs and sprays. For a leaf is

only a flat piece of radiation; but the tree throws its branches on all

sides, and even in every profile view of it, which presents a radiation

more or less correspondent to that of its leaves, it is more beautiful,

because varied by the freedom of the separate branches. I believe it has

been ascertained that, in all trees, the angle at which, in their

leaves, the lateral ribs are set on their central rib is approximately

the same at which the branches leave the great stem; and thus each

section of the tree would present a kind of magnified view of its own

leaf, were it not for the interfering force of gravity on the masses of

foliage. This force in proportion to their age, and the lateral

leverage upon them, bears them downwards at the extremities, so that, as

before noticed, the lower the bough grows on the stem, the more it

droops (Fig. 17, p. 67); besides this, nearly all beautiful trees have a

tendency to divide into two or more principal masses, which give a

prettier and more complicated symmetry than if one stem ran all the way

up the center. Fig. 41 may thus be considered the simplest type of tree

radiation, as opposed to leaf radiation. In this figure, however, all

secondary ramification is unrepresented, for the sake of simplicity; but

if we take one half of such a tree, and merely give two secondary

branches to each main branch (as represented in the general branch

structure shown at _b_, Fig. 18, p. 68), we shall have the form Fig. 42.

This I consider the perfect general type of tree structure; and it is

curiously connected with certain forms of Greek, Byzantine, and Gothic

ornamentation, into the discussion of which, however, we must not enter

here. It will be observed, that both in Figs. 41 and 42 all the branches

so spring from the main stem as very nearly to suggest their united

radiation from the root R. This is by no means universally the case; but

if the branches do not bend towards a point in the root, they at least

converge to some point or other. In the examples in Fig. 43, the

mathematical center of curvature, _a_, is thus, in one case, on the

ground, at some distance from the root, and in the other, near the top

of the tree. Half, only, of each tree is given, for the sake of

clearness: Fig. 44 gives both sides of another example, in which the

origins of curvature are below the root. As the positions of such points

may be varied without end, and as the arrangement of the lines is also

farther complicated by the fact of the boughs springing for the most

part in a spiral order round the tree, and at proportionate distances,

the systems of curvature which regulate the form of vegetation are quite

infinite. Infinite is a word easily said, and easily written, and people

do not always mean it when they say it; in this case I _do_ mean it: the

number of systems is incalculable, and even to furnish anything like a

representative number of types, I should have to give several hundreds

of figures such as Fig. 44.[60]

[Illustration: FIG. 43.]

[Illustration: FIG. 44.]

[Illustration: FIG. 45.]

211. Thus far, however, we have only been speaking of the great

relations of stem and branches. The forms of the branches themselves are

regulated by still more subtle laws, for they occupy an intermediate

position between the form of the tree and of the leaf. The leaf has a

flat ramification; the tree a completely rounded one; the bough is

neither rounded nor flat, but has a structure exactly balanced between

the two, in a half-flattened, half-rounded flake, closely resembling in

shape one of the thick leaves of an artichoke or the flake of a fir

cone; by combination forming the solid mass of the tree, as the leaves

compose the artichoke head. I have before pointed out to you the general

resemblance of these branch flakes to an extended hand; but they may be

more accurately represented by the ribs of a boat. If you can imagine a

very broad-headed and flattened boat applied by its keel to the end of a

main branch,[61] as in Fig. 45, the lines which its ribs will take,

supposing them outside of its timbers instead of inside, and the general

contour of it, as seen in different directions, from above and below,

will give you the closest approximation to the perspectives and

foreshortenings of a well-grown branch-flake. Fig. 25 above, p. 89, is

an unharmed and unrestrained shoot of healthy young oak; and, if you

compare it with Fig. 45, you will understand at once the action of the

lines of leafage; the boat only failing as a type in that its ribs are

too nearly parallel to each other at the sides, while the bough sends

all its ramification well forwards, rounding to the head, that it may

accomplish its part in the outer form of the whole tree, yet always

securing the compliance with the great universal law that the branches

nearest the root bend most back; and, of course, throwing _some_ always

back as well as forwards; the appearance of reversed action being much

increased, and rendered more striking and beautiful, by perspective.

Fig. 25 shows the perspective of such a bough as it is seen from below;

Fig. 46 gives rudely the look it would have from above.

[Illustration: FIG. 46.]

212. You may suppose, if you have not already discovered, what

subtleties of perspective and light and shade are involved in the

drawing of these branch-flakes, as you see them in different directions

and actions; now raised, now depressed: touched on the edges by the

wind, or lifted up and bent back so as to show all the white under

surfaces of the leaves shivering in light, as the bottom of a boat rises

white with spray at the surge-crest; or drooping in quietness towards

the dew of the grass beneath them in windless mornings, or bowed down

under oppressive grace of deep-charged snow. Snow time, by the way, is

one of the best for practice in the placing of tree masses; but you will

only be able to understand them thoroughly by beginning with a single

bough and a few leaves placed tolerably even, as in Fig. 38, p. 149.

First one with three leaves, a central and two lateral ones, as at _a_;

then with five, as at _b_, and so on; directing your whole attention to

the expression, both by contour and light and shade, of the boat-like

arrangements, which, in your earlier studies, will have been a good deal

confused, partly owing to your inexperience, and partly to the depth of

shade, or absolute blackness of mass required in those studies.

213. One thing more remains to be noted, and I will let you out of the

wood. You see that in every generally representative figure I have

surrounded the radiating branches with a dotted line: such lines do

indeed terminate every vegetable form; and you see that they are

themselves beautiful curves, which, according to their flow, and the

width or narrowness of the spaces they inclose, characterize the species

of tree or leaf, and express its free or formal action, its grace of

youth or weight of age. So that, throughout all the freedom of her

wildest foliage, Nature is resolved on expressing an encompassing limit;

and marking a unity in the whole tree, caused not only by the rising of

its branches from a common root, but by their joining in one work, and

being bound by a common law. And having ascertained this, let us turn

back for a moment to a point in leaf structure which, I doubt not, you

must already have observed in your earlier studies, but which it is well

to state here, as connected with the unity of the branches in the great

trees. You must have noticed, I should think, that whenever a leaf is

compound,--that is to say, divided into other leaflets which in any way

repeat or imitate the form of the whole leaf,--those leaflets are not

symmetrical, as the whole leaf is, but always smaller on the side

towards the point of the great leaf, so as to express their

subordination to it, and show, even when they are pulled off, that they

are not small independent leaves, but members of one large leaf.

214. Fig. 47, which is a block-plan of a leaf of columbine, without its

minor divisions on the edges, will illustrate the principle clearly. It

is composed of a central large mass, A, and two lateral ones, of which

the one on the right only is lettered, B. Each of these masses is again

composed of three others, a central and two lateral ones; but observe,

the minor one, _a_ of A, is balanced equally by its opposite; but the

minor _b_ 1 of B is larger than its opposite _b_ 2. Again, each of these

minor masses is divided into three; but while the central mass, A of A,

is symmetrically divided, the B of B is unsymmetrical, its largest

side-lobe being lowest. Again, in _b_ 2, the lobe _c_ 1 (its lowest lobe

in relation to B) is larger than _c_ 2; and so also in _b_ 1. So that

universally one lobe of a lateral leaf is always larger than the other,

and the smaller lobe is that which is nearer the central mass; the lower

leaf, as it were by courtesy, subduing some of its own dignity or power,

in the immediate presence of the greater or captain leaf, and always

expressing, therefore, its own subordination and secondary character.

This law is carried out even in single leaves. As far as I know, the

upper half, towards the point of the spray, is always the smaller; and a

slightly different curve, more convex at the springing, is used for the

lower side, giving an exquisite variety to the form of the whole leaf;

so that one of the chief elements in the beauty of every subordinate

leaf throughout the tree is made to depend on its confession of its own

lowliness and subjection.

[Illustration: FIG. 47.]

215. And now, if we bring together in one view the principles we have

ascertained in trees, we shall find they may be summed under four great

laws; and that all perfect[62] vegetable form is appointed to express

these four laws in noble balance of authority.

The Elements of Drawing, in Three Letters to Beginners · 第 42 / 71 题