CHAPTER I.

At the present time our actions are largely influenced by our theories.

We have abandoned the simple and instinctive mode of life of the earlier

civilisations for one regulated by the assumptions of our knowledge and

supplemented by all the devices of intelligence. In such a state it is

possible to conceive that a danger may arise, not only from a want of

knowledge and practical skill, but even from the very presence and

possession of them in any one department, if there is a lack of

information in other departments. If, for instance, with our present

knowledge of physical laws and mechanical skill, we were to build houses

without regard to the conditions laid down by physiology, we should

probably—to suit an apparent convenience—make them perfectly

draught-tight, and the best-constructed mansions would be full of

suffocating chambers. The knowledge of the construction of the body and

the conditions of its health prevent it from suffering injury by the

development of our powers over nature.

In no dissimilar way the mental balance is saved from the dangers

attending an attention concentrated on the laws of mechanical science by

a just consideration of the constitution of the knowing faculty, and the

conditions of knowledge. Whatever pursuit we are engaged in, we are

acting consciously or unconsciously upon some theory, some view of

things. And when the limits of daily routine are continually narrowed by

the ever-increasing complication of our civilisation, it becomes doubly

important that not one only but every kind of thought should be shared

in.

There are two ways of passing beyond the domain of practical certainty,

and of looking into the vast range of possibility. One is by asking,

“What is knowledge? What constitutes experience?” If we adopt this

course we are plunged into a sea of speculation. Were it not that the

highest faculties of the mind find therein so ample a range, we should

return to the solid ground of facts, with simply a feeling of relief at

escaping from so great a confusion and contradictoriness.

The other path which leads us beyond the horizon of actual experience is

that of questioning whatever seems arbitrary and irrationally limited in

the domain of knowledge. Such a questioning has often been successfully

applied in the search for new facts. For a long time four gases were

considered incapable of being reduced to the liquid state. It is but

lately that a physicist has succeeded in showing that there is no such

arbitrary distinction among gases. Recently again the question has been

raised, “Is there not a fourth state of matter?” Solid, liquid, and

gaseous states are known. Mr. Crookes attempts to demonstrate the

existence of a state differing from all of these. It is the object of

these pages to show that, by supposing away certain limitations of the

fundamental conditions of existence as we know it, a state of being can

be conceived with powers far transcending our own. When this is made

clear it will not be out of place to investigate what relations would

subsist between our mode of existence and that which will be seen to be

a possible one.

In the first place, what is the limitation that we must suppose away?

An observer standing in the corner of a room has three directions

naturally marked out for him; one is upwards along the line of meeting

of the two walls; another is forwards where the floor meets one of the

walls; a third is sideways where the floor meets the other wall. He can

proceed to any part of the floor of the room by moving first the right

distance along one wall, and then by turning at right angles and walking

parallel to the other wall. He walks in this case first of all in the

direction of one of the straight lines that meet in the corner of the

floor, afterwards in the direction of the other. By going more or less

in one direction or the other, he can reach any point on the floor, and

any movement, however circuitous, can be resolved into simple movements

in these two directions.

But by moving in these two directions he is unable to raise himself in

the room. If he wished to touch a point in the ceiling, he would have to

move in the direction of the line in which the two walls meet. There are

three directions then, each at right angles to both the other, and

entirely independent of one another. By moving in these three directions

or combinations of them, it is possible to arrive at any point in a

room. And if we suppose the straight lines which meet in the corner of

the room to be prolonged indefinitely, it would be possible by moving in

the direction of those three lines, to arrive at any point in space.

Thus in space there are three independent directions, and only three;

every other direction is compounded of these three. The question that

comes before us then is this. “Why should there be three and only three

directions?” Space, as we know it, is subject to a limitation.

In order to obtain an adequate conception of what this limitation is, it

is necessary to first imagine beings existing in a space more limited

than that in which we move. Thus we may conceive a being who has been

throughout all the range of his experience confined to a single straight

line. Such a being would know what it was to move to and fro, but no

more. The whole of space would be to him but the extension in both

directions of the straight line to an infinite distance. It is evident

that two such creatures could never pass one another. We can conceive

their coming out of the straight line and entering it again, but they

having moved always in one straight line, would have no conception of

any other direction of motion by which such a result could be effected.

The only shape which could exist in a one-dimensional existence of this

kind would be a finite straight line. There would be no difference in

the shapes of figures; all that could exist would simply be longer or

shorter straight lines.

Again, to go a step higher in the domain of a conceivable existence.

Suppose a being confined to a plane superficies, and throughout all the

range of its experience never to have moved up or down, but simply to

have kept to this one plane. Suppose, that is, some figure, such as a

circle or rectangle, to be endowed with the power of perception; such a

being if it moves in the plane superficies in which it is drawn, will

move in a multitude of directions; but, however varied they may seem to

be, these directions will all be compounded of two, at right angles to

each other. By no movement so long as the plane superficies remains

perfectly horizontal, will this being move in the direction we call up

and down. And it is important to notice that the plane would be

different, to a creature confined to it, from what it is to us. We think

of a plane habitually as having an upper and a lower side, because it is

only by the contact of solids that we realize a plane. But a creature

which had been confined to a plane during its whole existence would have

no idea of there being two sides to the plane he lived in. In a plane

there is simply length and breadth. If a creature in it be supposed to

know of an up or down he must already have gone out of the plane.

Is it possible, then, that a creature so circumstanced would arrive at

the notion of there being an up and down, a direction different from

those to which he had been accustomed, and having nothing in common with

them? Obviously nothing in the creature’s circumstances would tell him

of it. It could only be by a process of reasoning on his part that he

could arrive at such a conception. If he were to imagine a being

confined to a single straight line, he might realise that he himself

could move in two directions, while the creature in a straight line

could only move in one. Having made this reflection he might ask, “But

why is the number of directions limited to two? Why should there not be

three?”

A creature (if such existed), which moves in a plane would be much more

fortunately circumstanced than one which can only move in a straight

line. For, in a plane, there is a possibility of an infinite variety of

shapes, and the being we have supposed could come into contact with an

indefinite number of other beings. He would not be limited, as in the

case of the creature in a straight line, to one only on each side of

him.

It is obvious that it would be possible to play curious tricks with a

being confined to a plane. If, for instance, we suppose such a being to

be inside a square, the only way out that he could conceive would be

through one of the sides of the square. If the sides were impenetrable,

he would be a fast prisoner, and would have no way out.

What his case would be we may understand, if we reflect what a similar

case would be in our own existence. The creature is shut in in all the

directions he knows of. If a man is shut in in all the directions he

knows of, he must be surrounded by four walls, a roof and a floor. A

two-dimensional being inside a square would be exactly in the same

predicament that a man would be, if he were in a room with no opening on

any side. Now it would be possible to us to take up such a being from

the inside of the square, and to set him down outside it. A being to

whom this had happened would find himself outside the place he had been

confined in, and he would not have passed through any of the boundaries

by which he was shut in. The astonishment of such a being can only be

imagined by comparing it to that which a man would feel, if he were

suddenly to find himself outside a room in which he had been, without

having passed through the window, doors, chimney or any opening in the

walls, ceiling or floor.

Another curious thing that could be effected with a two-dimensional

being, is the following. Conceive two beings at a great distance from

one another on a plane surface. If the plane surface is bent so that

they are brought close to one another, they would have no conception of

their proximity, because to each the only possible movements would seem

to be movements in the surface. The two beings might be conceived as so

placed, by a proper bending of the plane, that they should be absolutely

in juxtaposition, and yet to all the reasoning faculties of either of

them a great distance could be proved to intervene. The bending might be

carried so far as to make one being suddenly appear in the plane by the

side of the other. If these beings were ignorant of the existence of a

third dimension, this result would be as marvellous to them, as it would

be for a human being who was at a great distance—it might be at the

other side of the world—to suddenly appear and really be by our side,

and during the whole time he not to have left the place in which he was.

CHAPTER II.

The foregoing examples make it clear that beings can be conceived as

living in a more limited space than ours. Is there a similar limitation

in the space we know?

At the very threshold of arithmetic an indication of such a limitation

meets us.

If there is a straight line before us two inches long, its length is

expressed by the number 2. Suppose a square to be described on the line,

the number of square inches in this figure is expressed by the number 4,

_i.e._, 2 × 2. This 2 × 2 is generally written 2², and named “2 square.”

Now, of course, the arithmetical process of multiplication is in no

sense identical with that process by which a square is generated from

the motion of a straight line, or a cube from the motion of a square.

But it has been observed that the units resulting in each case, though

different in kind, are the same in number.

If we touch two things twice over, the act of touching has been

performed four times. Arithmetically, 2 × 2 = 4. If a square is

generated by the motion of a line two inches in length, this square

contains four square inches.

So it has come to pass that the second and third powers of numbers are

called “square” and “cube.”

We have now a straight line two inches long. On this a square has been

constructed containing four square inches. If on the same line a cube be

constructed, the number of cubic inches in the figure so made is 8,

_i.e._, 2 × 2 × 2 or 2³. Here, corresponding to the numbers 2, 2², 2³,

we have a series of figures. Each figure contains more units than the

last, and in each the unit is of a different kind. In the first figure a

straight line is the unit, viz., one linear inch; it is said to be of

one dimension. In the second a square is the unit, viz., one square

inch. The square is a figure of two dimensions. In the third case a cube

is the unit, and the cube is of three dimensions. The straight line is

said to be of one dimension because it can be measured only in one way.

Its length can be taken, but it has no breadth or thickness. The square

is said to be of two dimensions because it has both length and breadth.

The cube is said to have three dimensions, because it can be measured in

three ways.

The question naturally occurs, looking at these numbers 2, 2², 2³, by

what figure shall we represent 2⁴, or 2 × 2 × 2 × 2. We know that in the

figure there must be sixteen units, or twice as many units as in the

cube. But the unit also itself must be different. And it must not differ

from a cube simply in shape. It must differ from a cube as a cube

differs from a square. No number of squares will make up a cube, because

each square has no thickness. In the same way, no number of cubes must

be able to make up this new unit. And here, instead of trying to find

something already known, to which the idea of a figure corresponding to

the fourth power can be affixed, let us simply reason out what the

properties of such a figure must be. In this attempt we have to rely,

not on a process of touching or vision, such as informs us of the

properties of bodies in the space we know, but on a process of thought.

Each fact concerning this unknown figure has to be reasoned out; and it

is only after a number of steps have been gone through, that any

consistent familiarity with its properties is obtained. Of all

applications of the reason, this exploration is perhaps the one which

requires, for the simplicity of the data involved, the greatest exercise

of the abstract imagination, and on this account is well worth patient

attention. The first steps are very simple. We must imagine a finite

straight line to generate a square by moving on the plane of the paper,

and this square in its turn to generate a cube by moving vertically

upwards. Fig. 1 represents a straight line; Fig. 2 represents a square

formed by the motion of that straight line; Fig. 3 represents

perspectively a cube formed by the motion of that square A B C D

upwards. It would be well, instead of using figure 3, to place a cube on

the paper. Its base would be A B C D, its upper surface E F G H.

[Illustration: Generating a line, square, and cube.]

The straight line A B gives rise to the square A B C D by a movement at

right angles to itself. If motion be confined to the straight line A B,

a backward and forward motion is the only one possible. No sideway

motion is admissible. And if we suppose a being to exist which could

only move in the straight line A B, it would have no idea of any other

movement than to and fro. The square A B C D is formed from the straight

line by a movement in a direction entirely different from the direction

which exists in A B. This motion is not expressible by means of any

possible motion in A B. A being which existed in A B, and whose

experience was limited to what could occur in A B, would not be able to

understand the instructions we should give to make A B trace out the

figure A B C D.

In the figure A B C D there is a possibility of moving in a variety of

directions, so long as all these directions are confined to one plane.

All directions in this plane can be considered as compounded of two,

from A to B, and from A to C. Out of the infinite variety of such

directions there is none which tends in a direction perpendicular to

Fig. 2; there is none which tends upwards from the plane of the paper.

Conceive a being to exist in the plane, and to move only in it. In all

the movements which he went through there would be none by which he

could conceive the alteration of Fig. 2 into what Fig. 3 represents in

perspective. For 2 to become 3 it must be supposed to move

perpendicularly to its own plane. The figure it traces out is the cube A

B C D E F G H.

All the directions, manifold as they are, in which a creature existing

in Fig. 3 could move, are compounded of three directions. From A to B,

from A to C, from A to E, and there are no other directions known to it.

But if we suppose something similar to be done to Fig. 3, something of

the same kind as was done to Fig. 1 to turn it into Fig. 2, or to Fig. 2

to turn it into Fig. 3, we must suppose the whole figure as it exists to

be moved in some direction entirely different from any direction within

it, and not made up of any combination of the directions in it. What is

this? It is the fourth direction.

We are as unable to imagine it as a creature living in the plane Fig. 2

would be to imagine a direction such that moving in it the square 2

would become the cube 3. The third dimension to such a creature would be

as unintelligible as the fourth is to us. And at this point we have to

give up the aid that is to be got from any presentable object, and we

have simply to investigate what the properties of the simplest figure in

four dimensions are, by pursuing further the analogy which we know to

exist between the process of formation of 2 from 1, and of 3 from 2, and

finally of 4 from 3. For the sake of convenience, let us call the figure

we are investigating—the simplest figure in four dimensions—a

four-square.

First of all we must notice, that if a cube be formed from a square by

the movement of the square in a new direction, each point of the

interior of the square traces out part of the cube. It is not only the

bounding lines that by their motion form the cube, but each portion of

the interior of the square generates a portion of the cube. So if a cube

were to move in the fourth dimension so as to generate a four-square,

every point in the interior of the cube would start _de novo_, and trace

out a portion of the new figure uninterfered with by the other points.

Or, to look at the matter in another light, a being in three dimensions,

looking down on a square, sees each part of it extended before him, and

can touch each part without having to pass through the surrounding

parts, for he can go from above, while the surrounding parts surround

the part he touches only in one plane.

So a being in four dimensions could look at and touch every point of a

solid figure. No one part would hide another, for he would look at each

part from a direction which is perfectly different from any in which it

is possible to pass from one part of the body to another. To pass from

one part of the body to another it is necessary to move in three

directions, but a creature in four dimensions would look at the solid

from a direction which is none of these three.

Let us obtain a few facts about the fourth figure, proceeding according

to the analogy that exists between 1, 2, 3, and 4. In the Fig. 1 there

are two points. In 2 there are four points—the four corners of the

square. In 3 there are eight points. In the next figure, proceeding

according to the same law, there would be sixteen points.

In the Fig. 1 there is one line. In the square there are four lines. In

the cube there are twelve lines. How many lines would there be in the

four-square? That is to say that there are three numbers—1, 4, and 12.

What is the fourth, going on accordingly to the same law?

To answer this question let us trace out in more detail how the figures

change into one another. The line, to become the square, moves; it

occupies first of all its original position, and last of all its final

position. It starts as A B, and ends as C D; thus the line appears

twice, or it is doubled. The two other lines in the square, A C, B D,

are formed by the motions of the points at the extremities of the moving

line. Thus, in passing from the straight line to the square the lines

double themselves, and each point traces out a line. If the same

procedure holds good in the case of the change of the square into the

cube, we ought in the cube to have double the number of lines as in the

square—that is eight—and every point in the square ought to become a

line. As there are four points in the square, we should have four lines

in the cube from them, that is, adding to the previous eight, there

should be twelve lines in the cube. This is obviously the case. Hence we

may with confidence, to deduce the number of lines in a four-square,

apply this rule. _Double the number of lines in the previous figure, and

add as many lines as there are points in the previous figure._ Now in

the cube there are twelve lines and eight points. Hence we get 2 × 12 +

8, or thirty-two lines in the four-square.

In the same way any other question about the four-square can be

answered. We must throw aside our realising power and answer in

accordance with the analogy to be worked out from the three figures we

know.

Thus, if we want to know how many plane surfaces the four-square has, we

must commence with the line, which has none; the square has one; the

cube has six. Here we get the three numbers, 0, 1, and 6. What is the

fourth?

Consider how the planes of the cube arise. The square at the beginning

of its motion determines one of the faces of the cube, at the end it is

the opposite face, during the motion each of the lines of the square

traces out one plane face of the cube. Thus we double the number of

planes in the previous figure, and every line in the previous figure

traces out a plane in the subsequent one.

Apply this rule to the formation of a square from a line. In the line

there is no plane surface, and since twice nothing is nothing, we get,

so far, no surface in the square; but in the straight line there is one

line, namely itself, and this by its motion traces out the plane surface

of the square. So in the square, as should be, the rule gives one

surface.

Applying this rule to the case of the cube, we get, doubling the

surfaces, 12; and adding a plane for each of the straight lines, of

which there are 12, we have another 12, or 24 plane surfaces in all.

Thus, just as by handling or looking at it, it is possible to describe a

figure in space, so by going through a process of calculation it is

within our power to describe all the properties of a figure in four

dimensions.

There is another characteristic so remarkable as to need a special

statement. In the case of a finite straight line, the boundaries are

points. If we deal with one dimension only, the figure 1, that of a

segment of a straight line, is cut out of and separated from the rest of

an imaginary infinitely long straight line by the two points at its

extremities. In this simple case the two points correspond to the

bounding surface of the cube. In the case of a two-dimensional figure an

infinite plane represents the whole of space. The square is separated

off by four straight lines, and it is impossible for an entry to be made

into the interior of the square, except by passing through the straight

lines. Now, in these cases, it is evident that the boundaries of the

figure are of one dimension less than the figure itself. Points bound

lines, lines bound plane figures, planes bound solid figures. Solids

then must bound four dimensional figures. The four-square will be

bounded in the following manner. First of all there is the cube which,

by its motion in the fourth direction, generates the figure. This, in

its initial position, forms the base of the four-square. In its final

position it forms the opposite end. During the motion each of the faces

of the cube give rise to another cube. The direction in which the cube

moves is such that of all the six sides none is in the least inclined in

that direction. It is at right angles to all of them. The base of the

cube, the top of the cube, and the four sides of the cube, each and all

of them form cubes. Thus the four-square is bounded by eight cubes.

Summing up, the four-square would have 16 points, 32 lines, 24 surfaces,

and it would be bounded by 8 cubes.

If a four-square were to rest in space it would seem to us like a cube.

To justify this conclusion we have but to think of how a cube would

appear to a two-dimensional being. To come within the scope of his

faculties at all, it must come into contact with the plane in which he

moves. If it is brought into as close a contact with this plane as

possible, it rests on it by one of its faces. This face is a square, and

the most a two-dimensional being could get acquainted with of a cube

would be a square.

Having thus seen how it is possible to describe the properties of the

simplest shape in four dimensions, it is evident that the mental

construction of more elaborate figures is simply a matter of time and

patience.

In the study of the form and development of the chick in the egg, it is

impossible to detect the features that are sought to be observed, except

by the use of the microscope. The specimens are accordingly hardened by

a peculiar treatment and cut into thin sections. The investigator going

over each of these sections, noticing all their peculiarities,

constructs in his mind the shape as it originally existed from the

record afforded by an indefinite number of slices. So, to form an idea

of a four-dimensional figure, a series of solid shapes bounded on every

side differing gradually from one another, proceeding, it may be, to the

most diverse forms, has to be mentally grasped and fused into a unitary

conception.

If, for instance, a small sphere were to appear, this to be replaced by

a larger one, and so on, and then, when the largest had appeared,

smaller and smaller ones to make their appearance, what would be

witnessed would be a series of sections of a four-dimensional sphere.

Each section in space being a sphere.

Again, just as solid figures can be represented on paper by perspective,

four-dimensional figures can be represented perspectively by solids. If

there are two squares, one lying over the other, and the underneath one

be pushed away, its sides remaining parallel with the one that was over

it, then if each point of the one be joined to the corresponding point

of the other, we have a fair representation on paper of a cube. Fig. 3

may be considered to be such a representation if the square C D G H be

considered to be the one that has been pushed away from lying originally

under the square A B E F. Each of the planes which bound the cube is

represented on the paper. The only thing that is wanting is the

three-dimensional content of the cube. So if two cubes be placed with

their sides parallel, but one somewhat diagonally with regard to the

other, and all their corresponding points be supposed joined, there will

be found a set of solid figures, each representing (though of course

distortedly) the bounding cubes of the four-dimensional figure, and

every plane and line in the four-dimensional figure will be found to be

represented in a kind of solid perspective. What is wanting is of course

the four-dimensional content.

CHAPTER III.

Having now passed in review some of the properties of four-dimensional

figures, it remains to ask what relations beings in four dimensions, if

they did exist, would have with us.

And in the first place, a being in four dimensions would have to us

exactly the appearance of a being in space. A being in a plane would

only know solid objects as two-dimensional figures—the shapes namely in

which they intersected his plane. So if there were four-dimensional

objects, we should only know them as solids—the solids, namely, in which

they intersect our space. Why, then, should not the four-dimensional

beings be ourselves, and our successive states the passing of them

through the three-dimensional space to which our consciousness is

confined?

Let us consider the question in more detail. And for the sake of

simplicity transfer the problem to the case of three and two dimensions

instead of four and three.

Suppose a thread to be passed through a thin sheet of wax placed

horizontally. It can be passed through in two ways. Either it can be

pulled through, or it can be held at both ends, and moved downwards as a

whole. Suppose a thread to be grasped at both ends, and the hands to be

moved downwards perpendicularly to the sheet of wax. If the thread

happens to be perpendicular to the sheet it simply passes through it,

but if the thread be held, stretched slantingwise to the sheet, and the

hands are moved perpendicularly downwards, the thread will, if it be

strong enough, make a slit in the sheet.

If now the sheet of wax were to have the faculty of closing up behind

the thread, what would appear in the sheet would be a moving hole.

Suppose that instead of a sheet and a thread, there were a straight line

and a plane. If the straight line were placed slantingwise in reference

to the plane and moved downwards, it would always cut the plane in a

point, but that point of section would move on. If the plane were of

such a nature as to close up behind the line, if it were of the nature

of a fluid, what would be observed would be a moving point. If now there

were a whole system of lines sloping in different directions, but all

connected together, and held absolutely still by one framework, and if

this framework with its system of lines were as a whole to pass slowly

through the fluid plane at right angles to it, there would then be the

appearance of a multitude of moving points in the plane, equal in number

to the number of straight lines in the system. The lines in the

framework will all be moving at the same rate—namely, at the rate of the

framework in which they are fixed. But the points in the plane will have

different velocities. They will move slower or faster, according as the

lines which give rise to them are more or less inclined to the plane. A

straight line perpendicular to the plane will, on passing through, give

rise to a stationary point. A straight line that slopes very much

inclined to the plane will give rise to a point moving with great

swiftness. The motions and paths of the points would be determined by

the arrangement of the lines in the system. It is obvious that if two

straight lines were placed lying across one another like the letter X,

and if this figure were to be stood upright and passed through the

plane, what would appear would be at first two points. These two points

would approach one another. When the part where the two strokes of the X

meet came into the plane, the two points would become one. As the upper

part of the figure passed through, the two points would recede from one

another.

[Illustration: Rectangle A B C D, crossed by two interlinked lines X

and Y two lines.]

If the line be supposed to be affixed to all parts of the framework, and

to loop over one another, and support one another,[1] it is obvious that

they could assume all sorts of figures, and that the points on the plane

would move in very complicated paths. The annexed figure represents a

section of such a framework. Two lines X X and Y Y are shown, but there

must be supposed to be a great number of others sloping backwards and

forwards as well as sideways.

Let us now assume that instead of lines, very thin threads were attached

to the framework: they on passing through the fluid plane would give

rise to very small spots. Let us call the spots atoms, and regard them

as constituting a material system in the plane. There are four

conditions which must be satisfied by these spots if they are to be

admitted as forming a material system such as ours. For the ultimate

properties of matter (if we eliminate attractive and repulsive forces,

which may be caused by the motions of the smallest particles), are—1,

Permanence; 2, Impenetrability; 3, Inertia; 4, Conservation of energy.

According to the first condition, or that of permanence, no one of these

spots must suddenly cease to exist. That is, the thread which by sharing

in the general motion of the system gives rise to the moving point, must

not break off before the rest of them. If all the lines suddenly ended

this would correspond to a ceasing of matter.

2. Impenetrability.—One spot must not pass through another. This

condition is obviously satisfied. If the threads do not coincide at any

point, the moving spots they give rise to cannot.

3. Inertia.—A spot must not cease to move or cease to remain at rest

without coming into collision with another point. This condition gives

the obvious condition with regard to the threads, that they, between the

points where they come into contact with one another, must be straight.

A thread which was curved would, passing through the plane, give rise to

a point which altered in velocity spontaneously. This the particles of

matter never do.

4. Conservation of energy.—The energy of a material system is never

lost; it is only transferred from one form to another, however it may

seem to cease. If we suppose each of the moving spots on the plane to be

the unit of mass, the principle of the conservation of energy demands

that when any two meet, the sum of the squares of their several

velocities before meeting shall be the same as the sum of the squares of

their velocities after meeting. Now we have seen that any statement

about the velocities of the spots in the plane is really a statement

about the inclinations of the threads to the plane. Thus the principle

of the conservation of energy gives a condition which must be satisfied

by the inclinations of the threads of the plane. Translating this

statement, we get in mathematical language the assertion that the sum of

the squares of the tangents of the angles the threads make with the

normal to the plane remains constant.

Hence, all complexities and changes of a material system made up of

similar atoms in a plane could result from the uniform motion as a whole

of a system of threads.

We can imagine these threads as weaving together to form connected

shapes, each complete in itself, and these shapes as they pass through

the fluid plane give rise to a series of moving points. Yet, inasmuch as

the threads are supposed to form consistent shapes, the motion of the

points would not be wholly random, but numbers of them would present the

semblance of moving figures. Suppose, for instance, a number of threads

to be so grouped as to form a cylinder for some distance, but after a

while to be pulled apart by other threads with which they interlink.

While the cylinder was passing through the plane, we should have in the

plane a number of points in a circle. When the part where the threads

deviated came to the plane, the circle would break up by the points

moving away. These moving figures in the plane are but the traces of the

shapes of threads as those shapes pass on. These moving figures may be

conceived to have a life and a consciousness of their own.

Or, if it be irrational to suppose them to have a consciousness when the

shapes of which they are momentary traces have none, we may well suppose

that the shapes of threads have consciousness, and that the moving

figures share this consciousness, only that in their case it is limited

to those parts of the shapes that simultaneously pass through the plane.

In the plane, then, we may conceive bodies with all the properties of a

material system, moving and changing, possessing consciousness. After a

while it may well be that one of them becomes so disassociated that it

appears no longer as a unit, and its consciousness as such may be lost.

But the threads of existence of such a figure are not broken, nor is the

shape which gave it origin altered in any way. It has simply passed on

to a distance from the plane. Thus nothing which existed in the

conscious life on the plane would cease. There would in such an

existence be no cause and effect, but simply the gradual realisation in

a superficies of an already existent whole. There would be no progress,

unless we were to suppose the threads as they pass to interweave

themselves in more complex shapes.

Can a representation, such as the preceding, be applied to the case of

the existence in space with which we have to do? Is it possible to

suppose that the movements and changes of material objects are the

intersections with a three-dimensional space of a four-dimensional

existence? Can our consciousness be supposed to deal with a spatial

profile of some higher actuality?

It is needless to say that all the considerations that have been brought

forward in regard to the possibility of the production of a system

satisfying the conditions of materiality by the passing of threads

through a fluid plane, holds good with regard to a four-dimensional

existence passing through a three-dimensional space. Each part of the

ampler existence which passed through our space would seem perfectly

limited to us. We should have no indication of the permanence of its

existence. Were such a thought adopted, we should have to imagine some

stupendous whole, wherein all that has ever come into being or will come

co-exists, which passing slowly on, leaves in this flickering

consciousness of ours, limited to a narrow space and a single moment, a

tumultuous record of changes and vicissitudes that are but to us. Change

and movement seem as if they were all that existed. But the appearance

of them would be due merely to the momentary passing through our

consciousness of ever existing realities.

In thinking of these matters it is hard to divest ourselves of the habit

of visual or tangible illustration. If we think of a man as existing in

four dimensions, it is hard to prevent ourselves from conceiving him as

prolonged in an already known dimension. The image we form resembles

somewhat those solemn Egyptian statues which in front represent well

enough some dignified sitting figure, but which are immersed to their

ears in a smooth mass of stone which fits their contour exactly.

No material image will serve. Organised beings seem to us so complete

that any addition to them would deface their beauty. Yet were we

creatures confined to a plane, the outline of a Corinthian column would

probably seem to be of a beauty unimprovable in its kind. We should be

unable to conceive any addition to it, simply for the reason that any

addition we could conceive would be of the nature of affixing an

unsightly extension to some part of the contour. Yet, moving as we do in

space of three dimensions, we see that the beauty of the stately column

far surpasses that of any single outline. So all that we can do is to

deny our faculty of judging of the ideal completeness of shapes in four

dimensions.

CHAPTER IV.

Let us now leave this supposition of framework and threads. Let us

investigate the conception of a four-dimensional existence in a simpler

and more natural manner—in the same way that a two-dimensional being

should think about us, not as infinite in the third dimension, but

limited in three dimensions as he is in two. A being existing in four

dimensions must then be thought to be as completely bounded in all four

directions as we are in three. All that we can say in regard to the

possibility of such beings is, that we have no experience of motion in

four directions. The powers of such beings and their experience would be

ampler, but there would be no fundamental difference in the laws of

force and motion.

Such a being would be able to make but a part of himself visible to us,

for a cube would be apprehended by a two-dimensional being as the square

in which it stood. Thus a four-dimensional being would suddenly appear

as a complete and finite body, and as suddenly disappear, leaving no

trace of himself, in space, in the same way that anything lying on a

flat surface, would, on being lifted, suddenly vanish out of the

cognisance of beings, whose consciousness was confined to the plane. The

object would not vanish by moving in any direction, but disappear

instantly as a whole. There would be no barrier, no confinement of our

devising that would not be perfectly open to him. He would come and go

at pleasure; he would be able to perform feats of the most surprising

kind. It would be possible by an infinite plane extending in all

directions to divide our space into two portions absolutely separated

from one another; but a four-dimensional being would slip round this

plane with the greatest ease.

To see this clearly, let us first take the analogous case in three

dimensions. Suppose a piece of paper to represent a plane. If it is

infinitely extended in every direction, it will represent an infinite

plane. It can be divided into two parts by an infinite straight line. A

being confined to this plane could not get from one part of it to the

other without passing through the line. But suppose another piece of

paper laid on the first and extended infinitely, it will represent

another infinite plane. If the being moves from the first plane by a

motion in the third dimension, it will move into this new plane. And in

it it finds no line. Let it move to such a position that when it goes

back to the first plane it will be on the other side of the line. Then

let it go back to the first plane. It has appeared now on the other side

of the line which divides the infinite plane into two parts.

Take now the case of four dimensions. Instead of bringing before the

mind a sheet of paper conceive a solid of three dimensions. If this

solid were to become infinite it would fill up the whole of

three-dimensional space. But it would not fill up the whole of

four-dimensional space. It would be to four-dimensional space what an

infinite plane is to three-dimensional space. There could be in

four-dimensional space an infinite number of such solids, just as in

three-dimensional space there could be an infinite number of infinite

planes.

Thus, lying alongside our space, there can be conceived a space also

infinite in all three directions. To pass from one to the other a

movement has to be made in the fourth dimension, just as to pass from

one infinite plane to another a motion has to be made in the third

dimension.

Conceive, then, corresponding to the first sheet of paper mentioned

above, a solid, and as the sheet of paper was supposed to be infinitely

extended in two dimensions, suppose the solid to be infinitely extended

in its three dimensions, so that it fills the whole of space as we know

it.

Now divide this infinite solid in two parts by an infinite plane, as the

infinite plane of paper was divided in two parts by an infinite line. A

being cannot pass from one part of this infinite solid to another, on

the other side of this infinite plane, without going through the

infinite plane, _so long as he keeps within the infinite solid_.

But suppose beside this infinite solid a second infinite solid, lying

next to it in the fourth dimension, as the second infinite plane of

paper was next to the first infinite plane in the third dimension. Let

now the being that wants to get on the other side of the dividing plane

move off in the fourth dimension, and enter the second infinite solid.

In this second solid there is no dividing plane. Let him now move, so

that coming back to the first infinite solid he shall be on the other

side of the infinite plane that divides it into two portions. If this is

done, he will now be on the other side of the infinite plane, without

having gone through it.

In a similar way a being, able to move in four dimensions, could get out

of a closed box without going through the sides, for he could move off

in the fourth dimension, and then move about, so that when he came back

he would be outside the box.

Is there anything in the world as we know it, which would indicate the

possibility of there being an existence in four dimensions? No definite

answer can be returned to this question. But it may be of some interest

to point out that there are certain facts which might be read by the

light of the fourth dimensional theory.

To make this clear, let us suppose that space is really four

dimensional, and that the three-dimensional space we know is, in this

ampler space, like a surface is in our space.

We should then be in this ampler space like beings confined to the

surface of a plane would be in ours. Let us suppose that just as in our

space there are centres of attraction whose influence radiates out in

every direction, so in this ampler space there are centres of attraction

whose influence radiates out in every direction. Is there anything to be

observed in nature which would correspond to the effect of a centre of

attraction lying out of our space, and acting on all the matter in it?

The effect of such a centre of attraction would not be to produce motion

in any known direction, because it does not lie off in any known

direction.

Let us pass to the corresponding case in three and two dimensions,

instead of four and three. Let us imagine a plane lying horizontally,

and in it some creatures whose experience was confined to it. If now

some water or other liquid were poured on to the plane, the creatures,

becoming aware of its presence, would find that it had a tendency to

spread out all over the plane. In fact it would not be to them as a

liquid is to us—it would rather correspond to a gas. For a gas, as we

know it, tends to expand in every direction, and gradually increase so

as to fill the whole of space. It exercises a pressure on the walls of

any vessel in which we confine it.

The liquid on the plane expands in all the dimensions which the

two-dimensional creatures on the plane know, and at the same time

becomes smaller in the third dimension, its absolute quantity remaining

unchanged. In like manner we might suppose that gases (which by

expansion become larger in the dimensions that we know) become smaller

in the fourth dimension.

The cause in this case would have to be sought for in an attractive

force, acting with regard to our space as the force of gravity acts with

regard to a horizontal plane.

Can we suppose that there is a centre of attraction somewhere off in the

fourth dimension, and that the gases, which we know are simply more

mobile liquids, expanding out in every direction under its influence.

This view receives a certain amount of support from the fact proved

experimentally that there is no absolute line of demarcation between a

liquid and a gas. The one can be made to pass into the other with no

moment intervening in which it can be said that now a change of state

has taken place.

We might then suppose that the matter we know extending in three

dimensions has also a small thickness in the fourth dimension; that

solids are rigid in the fourth as in the other three dimensions; that

liquids are too coherent to admit of their spreading out in space, and

becoming thinner in the fourth dimension, under the influence of an

attractive centre lying outside of our space; but that gases, owing to

the greater mobility of their particles, are subject to its action, and

spread out in space under its influence, in the same manner that

liquids, under the influence of gravity, spread out on a plane.

Then the density of a gas would be a measure of the relative thickness

of it in the fourth dimension: and the diminution of the density would

correspond to a diminution of the thickness in the fourth dimension.

Could this supposition be tested in any way?

Suppose a being confined to a plane; if the plane is moved far off from

the centre of attraction lying outside it, he would find that liquids

had less tendency to spread out than before.

Or suppose he moves to a distant part of the plane so that the line from

his position to the centre of attraction lies obliquely to the plane; he

would find that in this position a liquid would show a tendency to

spread out more in one direction than another.

Now our space considered as lying in four-dimensional space, as a plane

does in three-dimensional space, may be shifted. And the expansive force

of gases might be found to be different at different ages. Or, shifting

as we do our position in space during the course of the earth’s path

round the sun, there might arise a sufficient difference in our position

in space, with regard to the attractive centre, to make the expansive

force of gases different at different times of the year, or to cause

them to manifest a greater expansive force in one direction than in

another.

But although this supposition might be worked out at some length, it is

hard to suppose that it could afford any definite test of the physical

existence of a fourth dimension. No test has been discovered which is

decisive. And, indeed, before searching for tests, a theoretical point

of the utmost importance has to be settled. In discussing the

geometrical properties of straight lines and planes, we suppose them to

be respectively of one and two dimensions, and by so doing deny them any

real existence. A plane and a line are mere abstractions. Every portion

of matter is of three dimensions. If we consider beings on a plane not

as mere idealities, we must suppose them to be of some thickness. If

their experience is to be limited to a plane this thickness must be very

small compared to their other dimensions. Transferring our reasoning to

the case of four dimensions, we come to a curious result.

If a fourth dimension exists there are two possible alternatives.

One is, that there being four dimensions, we have a three-dimensional

existence only. The other is that we really have a four-dimensional

existence, but are not conscious of it. If we are in three dimensions

only, while there are really four dimensions, then we must be relatively

to those beings who exist in four dimensions, as lines and planes are in

relation to us. That is, we must be mere abstractions. In this case we

must exist only in the mind of the being that conceives us, and our

experience must be merely the thoughts of his mind—a result which has

apparently been arrived at, on independent grounds, by an idealist

philosopher.

The other alternative is that we have a four-dimensional existence. In

this case our proportions in it must be infinitely minute, or we should

be conscious of them. If such be the case, it would probably be in the

ultimate particles of matter, that we should discover the fourth

dimension, for in the ultimate particles the sizes in the three

dimensions are very minute, and the magnitudes in all four dimensions

would be comparable.

The preceding two alternative suppositions are based on the hypothesis

of the reality of four-dimensional existence, and must be conceived to

hold good only on that hypothesis.

It is somewhat curious to notice that we can thus conceive of an

existence relative to which that which we enjoy must exist as a mere

abstraction.

Apart from the interest of speculations of this kind they have

considerable value; for they enable us to express in intelligible terms

things of which we can form no image. They supply us, as it were, with

scaffolding, which the mind can make use of in building up its

conceptions. And the additional gain to our power of representation is

very great.

Many philosophical ideas and doctrines are almost unintelligible because

there is no physical illustration which will serve to express them. In

the imaginary physical existence which we have traced out, much that

philosophers have written finds adequate representation. Much of

Spinoza’s Ethics, for example, could be symbolized from the preceding

pages.

Thus we may discuss and draw perfectly legitimate conclusions with

regard to unimaginable things.

It is, of course, evident that these speculations present no point of

direct contact with fact. But this is no reason why they should be

abandoned. The course of knowledge is like the flow of some mighty

river, which, passing through the rich lowlands, gathers into itself the

contributions from every valley. Such a river may well be joined by a

mountain stream, which, passing with difficulty along the barren

highlands, flings itself into the greater river down some precipitous

descent, exhibiting at the moment of its union the spectacle of the

utmost beauty of which the river system is capable. And such a stream is

no inapt symbol of a line of mathematical thought, which, passing

through difficult and abstract regions, sacrifices for the sake of its

crystalline clearness the richness that comes to the more concrete

studies. Such a course may end fruitlessly, for it may never join the

main course of observation and experiment. But, if it gains its way to

the great stream of knowledge, it affords at the moment of its union the

spectacle of the greatest intellectual beauty, and adds somewhat of

force and mysterious capability to the onward current.

The Persian King.

_PART I._

CHAPTER I.

In Persia there was once a king. On one occasion when he was out hunting

he came to the narrow entrance of a valley. It was shut in on either

side by vast hills, seemingly the spurs from the distant mountains.

These great spurs spread out including a wide tract of land. Towards the

entrance where he stood they approached one another, and ended in abrupt

cliffs. Across the mouth of the valley stretched a deep ravine. The

king, followed by courtiers, galloped along, searching a spot where the

deep fissure might be shallower, so that descending into it he might

reach the valley by ascending on the opposite side.

But at every point the ravine stretched downwards dark and deep, from

cliff to cliff, shutting off all access to the valley.

At one point only was there a means of crossing. There were two masses

of rocks, jutting out one from either side like the abutments of a

natural bridge, and they seemed to meet in mid air.

The mass trembled and shook as the king spurred his horse over it, and

the dislodged stones reverberated from side to side of the chasm till

the noise of their falling was lost.

Before the first of his courtiers could follow him one of the great

piers or abutments gave way—the whole mass fell crashing down. The king

was alone in the valley.

“So ho,” he cried, “the kingdom of Persia is shrunk to this narrow

spot!” and without troubling himself for the moment how he should

return, he sped onward.

But when he had ridden far into the valley on his steed that could

outnumber ten leagues in an hour, and had returned to the entrance of

it, he saw no trace of a living soul on the opposite brink of the cleft.

No sign was left, save a few reeds bent down by the passage of the

mounted train, that any human being had stood on the opposite side for

ages.

The evening came on apace. Yet no one returned. Again he rode far into

the valley. For the most part it was covered with long grass, but here

and there a thick and tangled mass of vegetation attested to a great

luxuriance of soil, while the surface was intersected here and there

with rivulets of clear water, which finally lost their way in the dark

gorge over which he had just so rashly adventured. But on no side did

the steep cliffs offer any promise of escape.

When the night came on he stretched himself beneath one of the few trees

not far from the ravine, while his faithful horse stood tranquilly at

his head.

He did not awake till the moon had risen. But then suddenly he started

to his feet, and walking to the edge of the cleft, peered over to the

land from whence he had come. For he thought he heard sounds of some

kind that were not the natural ones of the rustling wind or the falling

water. Looking out he saw clearly opposite to him an old man in ragged

clothing, leaning against a rock, holding a long pipe in his hands, on

which he now and again played a few wild notes.

“Oho, peasant!” cried the king. “Run and tell the head man of your

village that the king bids him come directly, and will have him bring

with him the longest ropes and the strongest throwers under him.”

But the old man did not seem to give heed. Then the king cried,

“Hearken, old man, run quickly and tell your master that the king is

confined here, and will reward him beyond his dreams if he deliver him

quickly.”

Then the old man rose, and coming nearer to the edge of the ravine stood

opposite, still playing at intervals some notes on his long pipe. And

the king cried, “Canst thou hear? Dost thou dare to refuse to carry my

commands? For I am the king of Persia. Who art thou?”

Then the old man made answer, putting his pipe aside: “I am he who

appears only when a man has passed for ever beyond the ken of all that

have known him. I am Demiourgos, the maker of men.”

Then the king cried, “Mock me not, but obey my commands.”

The old man made answer, “I do not mock thee; and oh, my Lord, thou hast

moved the puppets I have made, and driven them so to dance on the

surface of the earth that I would willingly obey thee. But it is not

permitted me to pass between thee and the world of men thou hast known.”

Then the king was silent.

At length he said, “If thou art really what thou sayest, show me what

thou canst do; build me a palace.”

The old man lifted his pipe in both his trembling hands, and began to

blow.

It was a strange instrument, for it not only produced the shriller

sounds of the lute, and the piercing notes of the trumpet, but resounded

with the hollow booming of great organ pipes, and amongst all came ever

and again a sharp and sonorous clang as of some metal instrument

resounding when it was struck.

And then the king was as one who enjoys the delights of thought. For in

thought, delicate shades, impalpable nuances are ever passing. It is as

the blended strains of an invisible orchestra, but more subtle far, that

come and go in unexpected metres, and overwhelm you with their beauty

when all seemed silent. And lo, as the strains sound, outside—palpable,

large as the firmament, or real as the smallest thing you can take up

and know it is there—outside stands some existence revealed—to be known

and returned to for ever.

So the king, listening to this music, felt that something was rising

behind him. And turning, beheld course after course of a great building.

Almost as soon as he had looked it had risen completed, finished to the

last embossure on the windows, the tracery on the highest pinnacles. All

had happened while the old man was blowing on his pipe, and when he

ceased all was perfect.

And yet the appearance was very strange, for a finished and seemingly

habitable building rose out of waste unreclaimed soil, strewn with rocks

and barren. No dwellings were near the palace to wait on it, no roads

led to it or away from it.

“There should be houses around it, and roadways,” said the king; “make

them, and fields sown with corn, and all that is necessary for a state.”

Blowing on his pipe in regular recurrent cadences, the old man called up

houses close together, than scattered singly along roads which stretched

away into the distance, to be seen every here and there perfectly

clearly where they ascended a rising ground. And near at hand could be

distinguished fields of grain and pasture land.

Yet as the king turned to walk towards the new scene, the old man

laughed. “All this is a dream,” he cried; “so much I can do, but not at

once.” And breathing peals of music from his pipe, he said, “This can

be, but is not yet.”

“What,” asked the king, “is all a delusion?” and as he asked everything

sank down. There was no palace, no houses or fields, only the steep

precipice-locked valley, whither the king had ridden; and his horse

cowering behind him.

Then the king cried, “Thou art some moonstruck hermit, leading out a

life of folly alone. Get thee to the village thou knowest, and bring me

help.”

But the old man answered him saying, “Great king, I am bound to obey

thee, and all the creative might of my being I lay at thy feet; and lo,

in the midst of this valley I make for thee beings such as I can

produce. And all that thou hast seen is as nothing to what I can do for

thee. The depths of the starry heavens have no limit, nor what I do for

thee. Hast thou ever in thy life looked into the deep still ocean, and

lost thy sight in the unseen depths? Even so thou wilt find no end in

what I will give thee. Hast thou ever in thy life sought the depths of

thy love’s blue eyes, and found therein a world which stretched on

endlessly? Even so I bring all to thy feet. Now that all the gladness of

the world has departed from thee, behold, I am a more willing servant

than ever thou hast had.”

And again he played, and a hut rose up with a patch of cleared soil

around it, and a spring near by.

Then the king said, “Here will I dwell, and if I am to be cut off from

the rest of the world, I will lead a peaceful life in this valley.”

The sun was rising, the sounds had ceased, and the old man had

disappeared.

Scientific Romances (First Series) · 第 1 / 12 章