Looking at the Weisshorn through the Nicol, the glow of its

protuberance was strong or weak according to the position of the

prism. The summit also underwent striking changes. In one position

of the prism it exhibited a pale white against a dark background; in

the rectangular position it was a dark mauve against a light

background. The red of the Matterhorn changed in a similar manner;

but the whole mountain also passed through wonderful changes of

definition. The air at the time was filled with a silvery haze, in

which the Matterhorn almost disappeared. This could be wholly

quenched by the Nicol, and then the mountain sprang forth with

astonishing solidity and detachment from the surrounding air. The

changes of the Dom were still more wonderful. A vast amounts of light

could be removed from the sky behind it, for it occupied the position

of maximum polarisation. By a little practice with the Nicol it was

easy to render the extinction of the light, or its restoration, almost

instantaneous. When the sky was quenched, the four minor peaks and

buttresses, and the summit of the Dom, together with the shoulder of

the Alphubel, glowed as if set suddenly on fire. This was immediately

dimmed by turning the Nicol through an angle of 90°. It was not the

stoppage of the light of the sky behind the mountains alone which

produced this startling effect; the air between them and me was highly

opalescent, and the quenching of this intermediate glare augmented

remarkably the distinctness of the mountains.

On the morning of August 24 similar effects were finely shown. At 10

A.M. all three mountains, the Dom, the Matterhorn, and the Weisshorn,

were powerfully affected by the Nicol. But in this instance also, the

line drawn to the Dom being very nearly perpendicular to the solar

beams, the effects on this mountain were most striking. The grey

summit of the Matterhorn, at the same time, could scarcely be

distinguished from the opalescent haze around it; but when the Nicol

quenched the haze, the summit became instantly isolated, and stood out

in bold definition. It is to be remembered that in the production of

these effects the only things changed are the sky behind, and the

luminous haze in front of the mountains; that these are changed

because the light emitted from the sky and from the haze is plane

polarised light, and that the light from the snows and from the

mountains, being sensibly unpolarised, is not directly affected by the

Nicol. It will also be understood that it is not the interposition of

the haze _as an opaque body_ that renders the mountains indistinct, but

that it is the _light_ of the haze which dims and bewilders the eye, and

thus weakens the definition of objects seen through it.

These results have a direct bearing upon what artists call 'aerial

perspective.' As we look from the summit of Mont Blanc, or from a

lower elevation, at the serried crowd of peaks, especially if the

mountains be darkly coloured--covered with pines, for example--every

peak and ridge is separated from the mountains behind it by a thin

blue haze which renders the relations of the mountains as to distance

unmistakable. When this haze is regarded through the Nicol

perpendicular to the sun's rays, it is in many cases wholly quenched,

because the light which it emits in this direction is wholly

polarised. When this happens, aerial perspective is abolished, and

mountains very differently distant appear to rise in the same vertical

plane. Close to the Bel Alp for instance, is the gorge of the Massa,

and beyond the gorge is a high ridge darkened by pines. This ridge

may be projected upon the dark slopes at the opposite side of the

Rhone valley, and between both we have the blue haze referred to,

throwing the distant mountains far away. But at certain hours of the

day the haze may be quenched, and then the Massa ridge and the

mountains beyond the Rhone seem almost equally distant from the eye.

The one appears, as it were, a vertical continuation of the other. The

haze varies with the temperature and humidity of the atmosphere. At

certain times and places it is almost as blue as the sky itself; but

to see its colour, the attention must be withdrawn from the mountains

and from the trees which cover them. In point of fact, the haze is a

piece of more or less perfect sky; it is produced in the same manner,

and is subject to the same laws, as the firmament itself. We live _in_

the sky, not _under_ it.

These points were further elucidated by the deportment of the

selenite, plate, with which the readers of the foregoing pages

are so well acquainted. On some of the sunny days of August the

haze in the valley of the Rhone, as looked at from the Bel Alp,

was very remarkable. Towards evening the sky above the mountains

opposite to my place of observation yielded a series of the most

splendidly-coloured iris-rings; but on lowering the selenite until it

had the darkness of the pines at the opposite side of the Rhone

'valley, instead of the darkness of space, as a background, the

colours were not much diminished in brilliancy. I should estimate the

distance across the valley, as the crow flies, to the opposite

mountain, at nine miles; so that a body of air of this thickness can,

under favourable circumstances, produce chromatic effects of

polarisation almost as vivid as those produced by the sky itself.

Again: the light of a landscape, as of most other things, consists of

two parts; the one, coming purely from superficial reflection, is

always of the same colour as the light which falls upon the landscape;

the other part reaches us from a certain depth within the objects

which compose the landscape, and it is this portion of the total light

which gives these objects their distinctive colours. The white light

of the sun enters all substances to a certain depth, and is partly

ejected by internal reflection; each distinct substance absorbing and

reflecting the light, in accordance with the laws of its own molecular

constitution. Thus the solar light is _sifted_ by the landscape, which

appears in such colours and variations of colour as, after the sifting

process, reach the observer's eye. Thus the bright green of grass, or

the darker colour of the pine, never comes to us alone, but is always

mingled with an amounts of light derived from superficial reflection.

A certain hard brilliancy is conferred upon the woods and meadows by

this superficially-reflected light. Under certain circumstances, it

may be quenched by a Nicol's prism, and we then obtain the true colour

of the grass and foliage. Trees and meadows, thus regarded, exhibit a

richness and softness of tint which they never show as long as the

superficial light is permitted to mingle with the true interior

emission. The needles of the pines show this effect very well,

large-leaved trees still better; while a glimmering field of maize

exhibits the most extraordinary variations when looked at through the

rotating Nicol.

Thoughts and questions like those here referred to took me, in August

1869, to the top of the Aletschhorn. The effects described in the

foregoing paragraphs were for the most part reproduced on the summit

of the mountain. I scanned the whole of the sky with my Nicol. Both

alone, and in conjunction with the selenite, it pronounced the

perpendicular to the solar beams to be the direction of maximum

polarisation.

But at no portion of the firmament was the polarisation complete. The

artificial sky produced in the experiments recorded in the preceding

pages could, in this respect, be rendered far more perfect than the

natural one; while the gorgeous 'residual blue' which makes its

appearance when the polarisation of the artificial sky ceases to be

perfect, was strongly contrasted with the lack-lustre hue which, in

the case of the firmament, outlived the extinction of the brilliancy.

With certain substances, however, artificially treated, this dull

residue may also be obtained.

All along the arc from the Matterhorn to Mont Blanc the light of the

sky immediately above the mountains was powerfully acted upon by the

Nicol. In some cases the variations of intensity were astonishing. I

have already said that a little practice enables the observer to shift

the Nicol from one position to another so rapidly as to render the

alternative extinction and restoration of the light immediate. When

this was done along the arc to which I have referred, the alternations

of light and darkness resembled the play of sheet lightning behind the

mountains. There was an element of awe connected with the suddenness

with which the mighty masses, ranged along the line referred to,

changed their aspect and definition under the operation of the prism.

*****

The physical reason of the blueness of both natural and artificial

skies is, I trust, correctly given in the essay on the Scientific use

of the Imagination published in the second volume of these Fragments.

********************

V. ON DUST AND DISEASE.

[Footnote: A discourse delivered before the Royal Institution of Great

Britain, January 21, 1870.]

Experiments on Dusty Air.

SOLAR light, in passing through a dark room, reveals its track by

illuminating the dust floating in the air. 'The sun,' says Daniel

Culverwell, 'discovers atomes, though they be invisible by

candle-light, and makes them dance naked in his beams.'

In my researches on the decomposition of vapours by light, I was

compelled to remove these 'atoms' and this dust. It was essential that

the space containing the vapours should embrace no visible thing--that

no substance capable of scattering light in the slightest sensible

degree should, at the outset of an experiments, be found in the wide

'experimental tube' in which the vapour was enclosed.

For a long time I was troubled by the appearance there of floating

matter, which, though invisible in diffuse daylight, was at once

revealed by a powerfully condensed beam. Two U-tubes were placed in

succession in the path of the air, before it entered the liquid whose

vapour was to be carried into the experimental tube. One of the

U-tubes contained fragments of marble wetted with a strong solution of

caustic potash; the other, fragments of glass wetted with concentrated

sulphuric acid which, while yielding no vapour of its own, powerfully

absorbs the aqueous vapour of the air. [Footnote: The apparatus is

figured in Fig. 3.] To my astonishment, the air of the Royal

Institution, sent through these tubes at a rate sufficiently slow to

dry it, and to remove its carbonic acid, carried into the experimental

tube a considerable amounts of mechanically suspended matter, which

was illuminated when the beam passed through the tube. The effect was

substantially the same when the air was permitted to bubble through

the liquid acid, and through the solution of potash.

I tried to intercept this floating matter in various ways; and on

October 5, 1868, prior to sending the air through the drying

apparatus, it was carefully permitted to pass over the tip of a

spirit-lamp flame. The floating matter no longer appeared, having

been burnt up by the flame. It was therefore _organic matter_. I was

by no means prepared for this result; having previously thought that

the dust of our air was, in great part, inorganic and non-combustible.

[Footnote: According to an analysis kindly furnished to me by Dr.

Percy, the dust collected _from the walls_ of the British Museum

contains fully 50 per cent. of inorganic matter. I have every

confidence in the results of this distinguished chemist; they show

that the _floating_ dust of our rooms is, as it were, winnowed from the

heavier matter. As bearing directly upon this point I may quote the

following passage from Pasteur: 'Mais ici se présente une remarque: la

poussière que Pon trouve à la surface de tous les corps est soumise

constamment à des courants d'air, qui doivent soulever des particules

les plus légères, au nombre desquelles se trouvent, sans doute, de

préférence les corpuscules organisés, oeufs ou spores, moins lourds

généralement que les particules minérales.']

I had constructed a small gas-furnace, now much employed by chemists,

containing a platinum tube, which could be heated to vivid redness.

[Footnote: Pasteur was, I believe, the first to employ such a tube.]

The tube contained a roll of platinum gauze, which, while it permitted

the air to pass through it, ensured the practical contact of the dust

with the incandescent metal. The air of the laboratory was permitted

to enter the experimental tube, sometimes through the cold, and

sometimes through the heated, tube of platinum. In the first column

of the following fragment of a long table the quantity of air operated

on is expressed by the depression of the mercury gauge of the

air-pump. In the second column the condition of the platinum tube is

mentioned, and in the third the state of the air in the experimental

tube.

Quantity of air State of platinum tube State of experimental tube

15 inches Cold Full of particles.

30 inches Red-hot Optically empty.

The phrase 'optically empty' shows that when the conditions of perfect

combustion were present, the floating matter totally disappeared.

*****

In a cylindrical beam, which strongly illuminated the dust of the

laboratory, I placed an ignited spirit-lamp. Mingling with the flame,

and round its rim, were seen curious wreaths of darkness resembling an

intensely black smoke. On placing the flame at some distance below

the beam, the same dark masses stormed upwards. They were blacker

than the blackest smoke ever seen issuing from the funnel of a

steamer; and their resemblance to smoke was so perfect as to lead the

most practised observer to conclude that the apparently pure flame of

the alcohol lamp required but a beam of sufficient intensity to reveal

its clouds of liberated carbon. But is the blackness smoke? This

question presented itself in a moment and was thus answered: A red-hot

poker was placed underneath the beam: from it the black wreaths also

ascended. A large hydrogen flame was next employed, and it produced

those whirling masses of darkness, far more copiously than either the

spirit-flame or poker. Smoke was therefore out of the question.

[Footnote: In none of the public rooms of the United States where I

had the honour to lecture was this experiment made. The organic dust

was too scanty. Certain rooms in England--the Brighton Pavilion, for

example--also lack the necessary conditions.]

What, then, was the blackness? It was simply that of stellar space;

that is to say, blackness resulting from the absence from the track of

the beam of all matter competent to scatter its light. When the flame

was placed below the beam the floating matter was destroyed _in situ_;

and the air, freed from this matter, rose into the beam, jostled aside

the illuminated particles, and substituted for their light the

darkness due to its own perfect transparency. Nothing could more

forcibly illustrate the invisibility of the agent which renders all

things visible. The beam crossed, unseen, the black chasm formed by

the transparent air, while, at both sides of the gap, the thick-strewn

particles shone out like a luminous solid under the powerful

illumination.

It is not, however, necessary to burn the particles to produce a

stream of darkness. Without actual combustion, currents may be

generated which shall displace the floating matter, and appear dark

amid the surrounding brightness. I noticed this effect first on

placing a red-hot copper ball below the beam, and permitting it to

remain there until its temperature had fallen below that of boiling

water. The dark currents, though much enfeebled, were still produced.

They may also be produced by a flask filled with hot water.

To study this effect a platinum wire was stretched across the beam,

the two ends of the wire being connected with the two poles of a

voltaic battery. To regulate the strength of the current a rheostat

was placed in the circuit. Beginning with a feeble current the

temperature of the wire was gradually augmented; but long before it

reached the heat of ignition, a flat stream of air rose from it, which

when looked at edgeways appeared darker and sharper than one of the

blackest lines of Fraunhofer in the purified spectrum. Right and left

of this dark vertical band the floating matter rose upwards, bounding

definitely the non-luminous stream of air. What is the explanation?

Simply this: The hot wire rarefied the air in contact with it, but it

did not equally lighten the floating matter. The convection current

of pure air therefore passed upwards among the inert particles,

dragging them after it right and left, but forming between them an

impassable black partition. This elementary experiments enables us to

render an account of the dark currents produced by bodies at a

temperature below that of combustion.

But when the platinum wire is intensely heated, the floating matter is

not only displaced, but destroyed. I stretched a wire about 4 inches

long through the air of an ordinary glass shade resting on

cotton-wool, which also surrounded the rim. The wire being raised to

a white heat by an electric current, the air expanded, and some of it

was forced through the cotton-wool. When the current was interrupted,

and the air within the shade cooled, the returning air did not carry

motes along with it, being filtered by the wool. At the beginning of

this experiments the shade was charged with floating matter; at the

end of half an hour it was optically empty.

On the wooden base of a cubical glass shade, a cubic foot in volume,

upright supports were fixed, and from one support to the other 38

inches of platinum wire were stretched in four parallel lines. The

ends of the platinum wire were soldered to two stout copper wires

which passed through the base of the shade and could be connected with

a battery. As in the last experiments the shade rested upon

cotton-wool. A beam sent through the shade revealed the suspended

matter. The platinum wire was then raised to whiteness. In five

minutes there was a sensible diminution of the matter, and in ten

minutes it was totally consumed.

Oxygen, hydrogen, nitrogen, carbonic acid, so prepared as to exclude

all floating particles, produce, when poured or blown into the beam,

the darkness of stellar space. Coal-gas does the same. An ordinary

glass shade, placed in the air with its mouth downwards, permits the

track of the beam to be seen crossing it. When coal-gas or hydrogen

is allowed to enter the shade by a tube reaching to its top, the gas

gradually fills the shade from above downwards. As soon as it

occupies the space crossed by the beam, the luminous track is

abolished. Lifting the shade so as to bring the common boundary of

gas and air above the beam, the track flashes forth. After the shade

is full, if it be inverted, the pure gas passes upwards like a black

smoke among the illuminated particles.

The Germ Theory of Contagious Disease.

There is no respite to our contact with the floating matter of the

air; and the wonder is, not that we should suffer occasionally from

its presence, but that so small a portion of it, and even that but

rarely diffused over large areas, should appear to be deadly to man.

And what is this portion? It was some time ago the current belief

that epidemic diseases generally were propagated by a kind of malaria,

which consisted of organic matter in a state of motor-decay; that when

such matter was taken into the body through the lungs, skin, or

stomach, it had the power of spreading there the destroying process by

which itself had been assailed. Such a power was visibly exerted in

the case of yeast. A little leaven was seen to leaven the whole

lump--a mere speck of matter, in this supposed state of decomposition,

being apparently competent to propagate indefinitely its own decay.

Why should not a bit of rotten malaria act in a similar manner within

the human frame? In 1836 a very wonderful reply was given to this

question. In that year Cagniard de la Tour discovered the

yeast-plant--a living organism, which when placed in a proper medium

feeds, grows, and reproduces itself, and in this way carries on the

process which we name fermentation. By this striking discovery

fermentation was connected with organic growth.

Schwann, of Berlin, discovered the yeast-plant independently about the

same time; and in February, 1837, he also announced the important

result, that when a decoction of meat is effectually screened from

ordinary air, and supplied solely with calcined air, putrefaction

never sets in. Putrefaction, therefore, he affirmed to be caused, not

by the air, but by something which could be destroyed by a

sufficiently high temperature. The results of Schwann were confirmed

by the independent experiments of Helmholtz, Ure, and Pasteur, while

other methods, pursued by Schultze, and by Schroeder and Dusch, led to

the same result.

But as regards fermentation, the minds of chemists, influenced

probably by the great authority of Gay-Lussac, fell back upon the old

notion of matter in a state of decay. It was not the living

yeast-plant, but the dead or dying parts of it, which, assailed by

oxygen, produced the fermentation. Pasteur, however, proved the real

'ferments,' mediate or immediate, to be organised beings which find in

the reputed ferments their necessary food.

Side by side with these researches and discoveries, and fortified by

them and others, has run the germ theory of epidemic disease. The

notion was expressed by Kircher, and favoured by Linnaeus, that

epidemic diseases may be due to germs which float in the atmosphere,

enter the body, and produce disturbance by the development within the

body of parasitic life. The strength of this theory consists in the

perfect parallelism of the phenomena of contagious disease with those

of life. As a planted acorn gives birth to an oak, competent to

produce a whole crop of acorns, each gifted with the power of

reproducing its parent tree; and as thus from a single seedling a

whole forest may spring; so, it is contended, these epidemic diseases

literally plant their seeds, grow, and shake abroad new germs, which,

meeting in the human body their proper food and temperature, finally

take possession of whole populations. There is nothing to my

knowledge in pure chemistry which resembles the power of propagation

and self-multiplication possessed by the matter which produces

epidemic disease. If you sow wheat you do not get barley; if you sow

small-pox you do not get scarlet-fever, but small-pox indefinitely

multiplied, and nothing else. The matter of each contagious disease

reproduces itself as rigidly as if it were (as Miss Nightingale puts

it) dog or cat.

Parasitic Diseases of Silkworms. Pasteur's Researches.

It is admitted on all hands that some diseases are the product of

parasitic growth. Both in man and in lower creatures, the existence

of such diseases has been demonstrated. I am enabled to lay before

you an account of an epidemic of this kind, thoroughly investigated

and successfully combated by M. Pasteur. For fifteen years a plague

had raged among the silkworms of France. They had sickened and died

in multitudes, while those that succeeded in spinning their cocoons

furnished only a fraction of the normal quantity of silk. In 1853 the

silk culture of France produced a revenue of one hundred and thirty

millions of francs. During the twenty previous years the revenue had

doubled itself, and no doubt was entertained as to its further

augmentation. The weight of the cocoons produced in 1853 was

26,000,000 kilogrammes; in 1865 it had fallen to 4,000,000, the fall

entailing, in a single year, a loss of 100,000,000 francs.

Fragments of Science: A Series of Detached Essays, Addresses, and Reviews. V. 1-2 · 第 9 / 69 段