The first question that naturally arises is, Can small particles be

really proved to act in the manner indicated? No doubt of it. Each

one of you can submit the question to an experimental test. Water

will not dissolve resin, but spirit will, and when spirit which

holds resin in solution is dropped into water the resin immediately

separates in solid particles, which render the water milky. The

coarseness of this precipitate depends on the quantity of the

dissolved resin. You can cause it to separate in thick clots or in

exceedingly fine particles. Professor Brücke has given us the

proportions which produce particles particularly suited to our

present purpose. One gramme of clean mastic is dissolved in

eighty-seven grammes of absolute alcohol, and the transparent

solution is allowed to drop into a beaker containing clear water

kept briskly stirred. An exceedingly fine precipitate is thus

formed, which declares its presence by its action upon light.

Placing a dark surface behind the beaker, and permitting the light

to fall into it from the top or front, the medium is seen to be

distinctly blue. It is not, perhaps, so perfect a blue as I have

seen on exceptional days, this year, among the Alps, but it is a

very fair sky blue. A trace of soap in water gives a tint of blue.

London, and I fear Liverpool milk, makes an approximation to the

same color through the operation of the same cause; and Helmholtz

has irreverently disclosed the fact that a blue eye is simply a

turbid medium.

Numerous instances of the kind might be cited. The action of turbid

media upon light was fully and beautifully illustrated by Goethe,

who, though unacquainted with the undulatory theory, was led by his

experiments to regard the blue of the firmament as caused by an

illuminated turbid medium with the darkness of space behind it. He

describes glasses showing a bright yellow by transmitted, and a

beautiful blue by reflected light. Professor Stokes, who was

probably the first to discern the real nature of the action of small

particles on the waves of ether, describes a glass of a similar

kind. What artists call “chill” is no doubt an effect of this

description. Through the action of minute particles, the browns of a

picture often present the appearance of the bloom of a plum. By

rubbing the varnish with a silk handkerchief optical continuity is

established and the chill disappears.

Some years ago I witnessed Mr. Hirst experimenting at Zermatt on the

turbid water of the Visp, which was charged with the finely divided

matter ground down by the glaciers. When kept still for a day or so

the grosser matter sank, but the finer matter remained suspended,

and gave a distinctly blue tinge to the water. No doubt the blueness

of certain Alpine lakes is in part due to this cause. Professor

Roscoe has noticed several striking cases of a similar kind. In a

very remarkable paper the late Principal Forbes showed that steam

issuing from the safety valve of a locomotive, when favorably

observed, exhibits at a certain stage of its condensation the colors

of the sky. It is blue by reflected light, and orange or red by

transmitted light. The effect, as pointed out by Goethe, is to some

extent exhibited by peat smoke.

More than ten years ago I amused myself at Killarney, by observing

on a calm day, the straight smoke columns rising from the chimneys

of the cabins. It was easy to project the lower portion of a column

against a bright cloud. The smoke in the former case was blue, being

seen mainly by reflected light; in the latter case it was reddish,

being seen mainly by transmitted light. Such smoke was not in

exactly the condition to give us the glow of the Alps, but it was a

step in this direction. Brücke’s fine precipitate above referred to

looks yellowish by transmitted light, but by duly strengthening the

precipitate you may render the white light of noon as ruby colored

as the sun when seen through Liverpool smoke or upon Alpine

horizons.

I do not, however, point to the gross smoke arising from coal as an

illustration of the action of small particles, because such smoke

soon absorbs and destroys the waves of blue instead of sending them

to the eyes of the observer.

These multifarious facts, and numberless others which cannot now be

referred to, are explained by reference to the single principle that

where the scattering particles are small in comparison to the size

of the waves, we have in the reflected light a greater proportion of

the smaller waves, and in the transmitted light a greater proportion

of the larger waves, than existed in the original white light. The

physiological consequence is that in the one light blue is

predominant, and in the other light orange or red. And now let us

push our inquiries forward. Our best microscopes can readily reveal

objects not more than 1/50000 of an inch in diameter. This is less

than the length of a wave of red light. Indeed, a first-rate

microscope would enable us to discern objects not exceeding in

diameter the length of the smallest waves of the visible spectrum.

By the microscope, therefore, we can submit our particles to an

experimental test. If they are as large as the light-waves they will

infallibly be seen; and if they are not seen it is because they are

smaller.

I placed in the hands of our president a bottle containing Brücke’s

particles in greater number and coarseness than those examined by

Brücke himself. The liquid was a milky blue, and Mr. Huxley applied

to it his highest microscopic power. He satisfied me at the time

that had particles of even 1/100000 of an inch in diameter existed

in the liquid they could not have escaped detection. But no

particles were seen. Under the microscope the turbid liquid was not

to be distinguished from distilled water. Brücke, I may say, also

found the particles to be of ultra microscopic magnitude.

But we have it in our power to imitate far more closely than we have

hitherto done the natural conditions of this problem. We can

generate in air, as many of you know, artificial skies, and prove

their perfect identity with the natural one as regards the

exhibition of a number of wholly unexpected phenomena. By a

continuous process of growth, moreover, we are able to connect sky

matter, if I may use the term, with molecular matter on the one

side, and with molar matter, or matter in sensible masses, on the

other.

In illustration of this, I will take an experiment described by M.

Morren, of Marseilles, at the last meeting of the British

Association. Sulphur and oxygen combine to form sulphurous acid gas.

It is this choking gas that is smelt when a sulphur match is burnt

in air. Two atoms of oxygen and one of sulphur constitute the

molecule of sulphurous acid. Now it has been recently shown in a

great number of instances that waves of ether issuing from a strong

source, such as the sun or the electric light, are competent to

shake asunder the atoms of gaseous molecules. A chemist would call

this “decomposition” by light; but it behooves us, who are examining

the power and function of the imagination, to keep constantly before

us the physical images which we hold to underlie our terms.

Therefore I say, sharply and definitely, that the components of the

molecules of sulphurous acid are shaken asunder by the ether waves.

Enclosing the substance in a suitable vessel, placing it in a dark

room, and sending through it a powerful beam of light, we at first

see nothing; the vessel containing the gas is as empty as a vacuum.

Soon, however, along the track of the beam a beautiful sky-blue

color is observed, which is due to the liberated particles of

sulphur. For a time the blue grows more intense; it then becomes

whitish; and from a whitish blue it passes to a more or less perfect

white. If the action be continued long enough, we end by filling the

tube with a dense cloud of sulphur particles, which by the

application of proper means may be rendered visible.

Here, then, our ether waves untie the bond of chemical affinity, and

liberate a body—sulphur—which at ordinary temperatures is a solid,

and which therefore soon becomes an object of the senses. We have

first of all the free atoms of sulphur, which are both invisible and

incompetent to stir the retina sensibly with scattered light. But

these atoms gradually coalesce and form particles, which grow larger

by continual accretion until after a minute or two they appear as

sky matter. In this condition they are invisible themselves, but

competent to send an amount of wave motion to the retina sufficient

to produce the firmamental blue. The particles continue, or may be

caused to continue, in this condition for a considerable time,

during which no microscope can cope with them. But they continually

grow larger, and pass by insensible gradations into the state of

_cloud_, when they can no longer elude the armed eye. Thus, without

solution of continuity, we start with matter in the molecule, and

end with matter in the mass, sky matter being the middle term of the

series of transformations.

Instead of sulphurous acid we might choose from a dozen other

substances, and produce the same effect with any of them. In the

case of some—probably in the case of all—it is possible to preserve

matter in the skyey condition for fifteen or twenty minutes under

the continual operation of the light. During these fifteen or twenty

minutes the particles are constantly growing larger, without ever

exceeding the size requisite to the production of the celestial

blue. Now when two vessels are placed before you, each containing

sky matter, it is possible to state with great distinctness which

vessel contains the largest particles.

The eye is very sensitive to differences of light, when, as here,

the eye is in comparative darkness, and when the quantities of wave

motion thrown against the retina are small. The larger particles

declare themselves by the greater whiteness of their scattered

light. Call now to mind the observation, or effort at observation,

made by our president when he failed to distinguish the particles of

resin in Brücke’s medium, and when you have done so follow me. I

permitted a beam of light to act upon a certain vapor. In two

minutes the azure appeared, but at the end of fifteen minutes it had

not ceased to be azure. After fifteen minutes, for example, its

color and some other phenomena pronounced it to be a blue of

distinctly smaller particles than those sought for in vain by Mr.

Huxley. These particles, as already stated, must have been less than

1/100000 of an inch in diameter.

And now I want you to submit to your imagination the following

question: Here are particles which have been growing continually for

fifteen minutes, and at the end of that time are demonstrably

smaller than those which defied the microscope of Mr. Huxley. What

must have been the size of these particles at the beginning of their

growth? What notion can you form of the magnitude of such particles?

As the distances of stellar space give us simply a bewildering sense

of vastness without leaving any distinct impression on the mind, so

the magnitudes with which we have here to do impress us with a

bewildering sense of smallness. We are dealing with infinitesimals

compared with which the test objects of the microscope are literally

immense.

From their perviousness to stellar light, and other considerations,

Sir John Herschel drew some startling conclusions regarding the

density and weight of comets. You know that these extraordinary and

mysterious bodies sometimes throw out tails 100,000,000 of miles in

length, and 50,000 miles in diameter. The diameter of our earth is

8,000 miles. Both it and the sky, and a good portion of space beyond

the sky, would certainly be included in a sphere 10,000 miles

across. Let us fill this sphere with cometary matter, and make it

our unit of measure. An easy calculation informs us that to produce

a comet’s tail of the size just mentioned, about 300,000 such

measures would have to be emptied into space. Now suppose the whole

of this stuff to be swept together, and suitably compressed, what do

you suppose its volume would be? Sir John Herschel would probably

tell you that the whole mass might be carted away at a single effort

by one of your dray-horses. In fact, I do not know that he would

require more than a small fraction of a horse-power to remove the

cometary dust. After this you will hardly regard as monstrous a

notion I have sometimes entertained concerning the quantity of

matter in our sky. Suppose a shell, then, to surround the earth at a

hight above the surface which would place it beyond the grosser

matter that hangs in the lower regions of the air—say at the hight

of the Matterhorn or Mont Blanc. Outside this shell we have the deep

blue firmament. Let the atmospheric space beyond the shell be swept

clean, and let the sky matter be properly gathered up. What is its

probable amount? I have sometimes thought that a lady’s portmanteau

would contain it all. I have thought that even a gentleman’s

portmanteau—possibly his snuff-box—might take it in. And whether the

actual sky be capable of this amount of condensation or not, I

entertain no doubt that a sky quite as vast as ours, and as good in

appearance, could be formed from a quantity of matter which might be

held in the hollow of the hand.

Small in mass, the vastness in point of number of the particles of

our sky may be inferred from the continuity of its light. It is not

in broken patches nor at scattered points that the heavenly azure is

revealed. To the observer on the summit of Mont Blanc the blue is as

uniform and coherent as if it formed the surface of the most

close-grained solid. A marble dome would not exhibit a stricter

continuity. And Mr. Glaisher will inform you that if our

hypothetical shell were lifted to twice the hight of Mont Blanc

above the earth’s surface, we should still have the azure overhead.

Everywhere through the atmosphere those sky particles are strewn.

They fill the Alpine valleys, spreading like a delicate gauze in

front of the slopes of pine. They sometimes so swathe the peaks with

light as to abolish their definition. This year I have seen the

Weisshorn thus dissolved in opalescent air.

By proper instruments the glare thrown from the sky particles

against the retina may be quenched, and then the mountain which it

obliterated starts into sudden definition. Its extinction in front

of a dark mountain resembles exactly the withdrawal of a veil. It is

the light then taking possession of the eye, and not the particles

acting as opaque bodies, that interfere with the definition.

By day this light quenches the stars; even by moonlight it is able

to exclude from vision all stars between the fifth and the eleventh

magnitude. It may be likened to a noise, and the stellar radiance to

a whisper drowned by the noise. What is the nature of the particles

which shed this light? On points of controversy I will not here

enter, but I may say that De la Rive ascribes the haze of the Alps

in fine weather to floating organic germs. Now the possible

existence of germs in such profusion has been held up as an

absurdity. It has been affirmed that they would darken the air, and

on the assumed impossibility of their existence in the requisite

numbers, without invasion of the solar light, a powerful argument

has been based by believers in spontaneous generation.

Similar arguments have been used by the opponents of the germ theory

of epidemic disease, and both parties have triumphantly challenged

an appeal to the microscope and the chemist’s balance to decide the

question. Without committing myself in the least to De la Rive’s

notion, without offering any objection here to the doctrine of

spontaneous generation, without expressing any adherence to the germ

theory of disease, I would simply draw attention to the fact that in

the atmosphere we have particles which defy both the microscope and

the balance, which do not darken the air, and which exist,

nevertheless, in multitudes sufficient to reduce to insignificance

the Israelitish hyperbole regarding the sands upon the seashore.

The varying judgments of men on these and other questions may

perhaps be, to some extent, accounted for by that doctrine of

relativity which plays so important a part in philosophy. This

doctrine affirms that the impressions made upon us by any

circumstance, or combination of circumstances, depends upon our

previous state. Two travelers upon the same peak, the one having

ascended to it from the plain, the other having descended to it from

a higher elevation, will be differently affected by the scene around

them. To the one nature is expanding, to the other it is

contracting, and feelings are sure to differ which have two such

different antecedent states.

In our scientific judgments the law of relativity may also play an

important part. To two men, one educated in the school of the

senses, who has mainly occupied himself with observation, and the

other educated in the school of imagination as well, and exercised

in the conception of atoms and molecules to which we have so

frequently referred, a bit of matter, say 1/50000 of an inch in

diameter, will present itself differently. The one descends to it

from his molar hights, the other climbs to it from his molecular

lowlands. To the one it appears small, to the other large. So also

as regards the appreciation of the most minute forms of life

revealed by the microscope. To one of these men they naturally

appear conterminous with the ultimate particles of matter, and he

readily figures the molecules from which they directly spring; with

him there is but a step from the atom to the organism. The other

discerns numberless organic gradations between both. Compared with

his atoms, the smallest vibrios and bacteria of the microscopic

field are as behemoth and leviathan.

The law of relativity may to some extent explain the different

attitudes of these two men with regard to the question of

spontaneous generation. An amount of evidence which satisfies the

one entirely fails to satisfy the other; and while to the one the

last bold defense and startling expansion of the doctrine will

appear perfectly conclusive, to the other it will present itself as

imposing a profitless labor of demolition on subsequent

investigators. The proper and possible attitude of these two men is

that each of them should work as if it were his aim and object to

establish the view entertained by the other.

I trust, Mr. President, that you—whom untoward circumstances have

made a biologist, but who still keep alive your sympathy with that

class of inquiries which nature intended you to pursue and

adorn—will excuse me to your brethren if I say that some of them

seem to form an inadequate estimate of the distance which separates

the microscopic from the molecular limit, and that, as a

consequence, they sometimes employ a phraseology which is calculated

to mislead.

When, for example, the contents of a cell are described as perfectly

homogeneous, as absolutely structureless, because the microscope

fails to distinguish any structure, then I think the microscope

begins to play a mischievous part. A little consideration will make

it plain to all of you that the microscope can have no voice in the

real question of germ structure. Distilled water is more perfectly

homogeneous than the contents of any possible organic germ. What

causes the liquid to cease contracting at 39° F., and to grow bigger

until it freezes? It is a structural process of which the microscope

can take no note, nor is it likely to do so by any conceivable

extension of its powers. Place this distilled water in the field of

an electro-magnet, and bring a microscope to bear upon it. Will any

change be observed when the magnet is excited? Absolutely none; and

still profound and complex changes have occurred.

First of all, the particles of water are rendered diamagnetically

polar; and secondly, in virtue of the structure impressed upon it by

the magnetic strain of its molecules, the liquid twists a ray of

light in a fashion perfectly determinate both as to quantity and

direction. It would be immensely interesting to both you and me if

one here present, who has brought his brilliant imagination to bear

upon this subject, could make us see as he sees the entangled

molecular processes involved in the rotation of the plane of

polarization by magnetic force. While dealing with this question he

lived in a world of matter and of motion to which the microscope has

no passport, and in which it can offer no aid. The cases in which

similar conditions hold are simply numberless. Have the diamond, the

amethyst, and the countless other crystals formed in the

laboratories of nature and of man, no structure? Assuredly they

have, but what can the microscope make of it? Nothing. It cannot be

too distinctly borne in mind that between the microscopic limit and

the true molecular limit there is room for infinite permutations and

combinations. It is in this region that the poles of the atoms are

arranged, that tendency is given to their powers, so that when these

poles and powers have free action and proper stimulus in a suitable

environment, they determine first the germ and afterwards the

complete organism. This first marshaling of the atoms on which all

subsequent action depends baffles a keener power than that of the

microscope. Through pure excess of complexity, and long before

observation can have any voice in the matter, the most highly

trained intellect, the most refined and disciplined imagination,

retires in bewilderment from the contemplation of the problem. We

are struck dumb by an astonishment which no microscope can relieve,

doubting not only the power of our instrument, but even whether we

ourselves possess the intellectual elements which will ever enable

us to grapple with the ultimate structural energies of nature.

But the speculative faculty, of which imagination forms so large a

part, will nevertheless wander into regions where the hope of

certainty would seem to be entirely shut out. We think that though

the detailed analysis may be, and may ever remain, beyond us,

general notions may be attainable. At all events, it is plain that

beyond the present outposts of microscopic inquiry lies an immense

field for the exercise of the imagination. It is only, however, the

privileged spirits who know how to use their liberty without abusing

it, who are able to surround imagination by the firm frontiers of

reason, that are likely to work with any profit here. But freedom to

them is of such paramount importance that, for the sake of securing

it, a good deal of wildness on the part of weaker brethren may be

overlooked. In more senses than one Mr. Darwin has drawn heavily

upon the scientific tolerance of his age. He has drawn heavily upon

_time_ in his development of species, and he has drawn adventurously

upon _matter_ in his theory of pan-genesis. According to this

theory, a germ already microscopic is a world of minor germs. Not

only is the organism as a whole wrapped up in the germ, but every

organ of the organism has there its special seed.

This, I say, is an adventurous draft on the power of matter to

divide itself and distribute its forces. But, unless we are

perfectly sure that he is overstepping the bounds of reason, that he

is unwittingly sinning against observed fact or demonstrated law—for

a mind like that of Darwin can never sin wittingly against either

fact or law—we ought, I think, to be cautious in limiting his

intellectual horizon. If there be the least doubt in the matter, it

ought to be given in favor of the freedom of such a mind. To it a

vast possibility is in itself a dynamic power, though the

possibility may never be drawn upon.

It gives me pleasure to think that the facts and reasonings of this

discourse tend rather towards the justification of Mr. Darwin than

towards his condemnation, that they tend rather to augment than to

diminish the cubic space demanded by this soaring speculator; for

they seem to show the perfect competence of matter and force, as

regards divisibility and distribution, to bear the heaviest strain

that he has hitherto imposed upon them.

Half Hours With Modern Scientists: Lectures and Essays · 第 18 / 19 段