CHAPTER VII.

LIGHT.

Theories of the Nature of Light--Hypotheses of Newton

and Huygens--Sources of Light--The Sun--Velocity of

Light--Transparency--Dark Lines of the Spectrum--Absorption

of Light--Colour--Prismatic Analysis--Rays of the

Spectrum--Rainbow--Diffraction--Interference--Goethe’s

Theory--Polarisation--Magnetisation of Light--Vision--The

Eye--Analogy--Sound and Light--Influence of Light on Animals and

Vegetables--Phosphorescence arising from several Causes--Artificial

Light--Its Colour dependent on Matter.

Light, the first creation, presents to the enquiring mind a series

of phenomena of the most exalted character. The glowing sunshine,

painting the earth with all the brilliancy of colour, and giving to the

landscape the inimitable charm of every degree of illumination, from

the grey shadow to the golden glow;--the calm of evening, when, weary

of the “excess of splendour,” the eye can repose in tranquillity upon

the “cloud-land” of the west, and watch the golden and the ruddy hues

fade slowly into the blue tincture of night;--and the pale refulgence

of the moon, with the quiet sparkle of the sun-lit stars,--all tend

to impress upon the soul, the great truth that, where there is light,

organisation and life are found, and beyond its influence death and

silence hold supreme dominion.[84] Through all time we have evidences

that this has been the prevailing feeling of the human race, derived,

of course, from their observation of the natural phenomena dependent

upon luminous agency. In the myths of every country, impersonations of

light prevail, and to these are referred the mysteries of the perpetual

renewal of life on the surface of the earth.

This presentiment of a philosophic truth, in the instance of the poet

sages of intellectual Greece, was advanced to the highest degree of

refinement; and the sublime exclamation of Plato: “Light is truth, and

God is light,” approaches nearly to a divine revelation.

As the medium of vision--as the cause of colour--as a power influencing

in a most striking manner all the forms of organisation around us,

light presented to the inquiring minds of all ages a subject of the

highest interest.

The ancient philosophers, although they lost themselves in the

metaphysical subtleties of their schools, could not but discover in

light an element of the utmost importance in natural operations. The

alchemists regarded the luminous principle as a most subtile fluid,

capable of interpenetrating and mingling with gross matter: gold

being supposed to differ from the baser metals only in containing a

larger quantity of this ethereal essence.[85] Modern science, after

investigating most attentively a greater number of the phenomena of

light, has endeavoured to assist the inquiry by the aid of hypotheses.

Newton, in a theory, which exhibits the refined character of that

great philosopher’s mind, supposes luminous particles to dart from the

surfaces of bodies in all directions--that these infinitely minute

particles are influenced by the attracting and repelling forces of

matter, and thus turned back, or reflected, from their superficies in

some cases, and absorbed into their interstitial spaces in others.

Huyghens, on the contrary, supposes light to be caused by the waves or

vibrations of an infinitely elastic medium--ETHER--diffused through all

space, which waves are propagated in every direction from the luminous

body. In the first theory, a luminous particle is supposed actually to

come from the sun to the earth; in the other, the sun only occasions a

disturbance of the _ether_, which extends with great rapidity, in the

same manner as a wave spreads itself over the surface of a lake.

Nearly all the facts known in the time of Newton, and those discovered

by him, were explained most satisfactorily by his hypothesis; but

it was found they could be interpreted equally as the effects of

undulation, with the exception of the production of colour by prismatic

refraction. Although the labours of many gifted minds have been given,

with the utmost devotion, to the support of the vibratory theory,

this simple fact has never yet received any satisfactory explanation;

and there are numerous discoveries connected with the molecular and

chemical disturbances produced by the sun’s rays, which do not appear

to be explained by the hypothesis of emission or of undulation.

In both theories a wave motion is admitted, and every fact renders

it probable that this mode of progression applies not only to light,

but to the so-called _imponderable forces_ in general. Admitting,

therefore, the undulatory movement of luminous rays, we shall not stop

to consider those points of the discussion which have been so ably

dealt with by Young, Laplace, Fresnel, Biot, Fraunhofer, Herschel,

Brewster, and others, but proceed at once to consider the sources of

light, and its more remarkable phenomena.[86]

The sun is the greatest permanently luminous body we are acquainted

with, and that orb is continually pouring off light from its surface

in all directions at the rate, through the resisting medium of space

and of our own atmosphere, of 192,000 miles in a second of time. It has

been calculated, however, that light would move through a vacuum with

the speed of 192,500 miles in the same period. We, therefore, learn

that a ray of light requires eight minutes and thirteen seconds to

come from the sun to us. In travelling from the distant planet Uranus,

nearly three hours are exhausted; and from the nearest of the fixed

stars each ray of light requires more than six years to traverse the

intervening space between it and the earth. Allow the mind to advance

to the regions of nebulæ, and it will be found that hundreds of years

must glide away during the passage of their radiations. Consequently,

if one of those masses of matter, or even one of the remote fixed

stars, was “blotted out of heaven” to-day, several generations of

the finite inhabitants of this world would fade out of time before

the obliteration could be known to man. Here the immensity of space

assists us in our conception, limited though it be, of the for-ever of

eternity.[87]

All the planets of our system shine with reflected light, and the

moon, our satellite, also owes her silvery lustre to the sun’s

radiations. The fixed stars are, in all probability, suns shining from

the far distance of space, with their own self-emitted lights. By the

photometric researches of Dr. Wollaston, we learn, however, that it

would take 20,000 millions of such orbs as Sirius, the brightest of the

fixed stars, to afford as much light as we derive from the sun. The

same observer has proved that the brightest effulgence of the full moon

is yet 801,072 times less than the luminous power of our solar centre.

The cultivators of modern science are a bold race; not contented with

endeavouring to understand the physical earth, they are endeavouring

to comprehend the condition of the solar surface. The mind of man can

penetrate far into nature, and, as it were, feel out the mysteries of

untraversed space. The astronomer learns of a peculiar condition of

light, which is termed polarisation, and he learns by this, too, that

he can determine if from a bright luminous disc the light is derived

from a solid mass in a state of intense ignition, or from vapour in

an incandescent condition. He adds a polarising apparatus to his

telescopes, and he determines that the light we derive from the sun

is due to an envelope of vapour--burning, in all probability--only

with greater intensity, as the gas which we now employ. This

_Photosphere_--as it has been called by the late French philosopher

Arago, is found to be subjected to violent disturbances, and the dark

spots seen on the sun’s disc are now known to be openings through this

mysterious envelope of light, which enable us to look in upon the dark

body of the sun itself.

Luminous phenomena may be produced by various means--chemical action

is a source of light; and, under several circumstances in which the

laws of affinity are strongly exerted, a very intense luminous effect

is produced. Under this head all the phenomena of combustion are

included. In the electric spark we have the development of light;

and the arc which is formed between charcoal points at the poles of

a powerful voltaic battery affords us the most intense artificial

illumination with which we are acquainted. In addition to these, we

have the peculiar phenomena of phosphorescence arising from chemical,

calorific, electrical, actinic, and vital excitation, all of which must

be particularly examined.

From whatever source we procure light, it is the same in character,

differing only in intensity. In its action upon matter, we have the

phenomena of transmission, of reflection, of refraction, of colour, of

polarisation, and of vision, to engage our attention.

A beam of white light falls upon a plate of colourless glass, and it

passes freely through it, losing but little of its intensity; the

largest portion being lost by reflection from the first surface upon

which the light impinges. If the glass is roughened by grinding, we

lose more light by absorption and by reflection from the asperities of

the roughened surface; but if we cover that face with any oleaginous

fluid, as, for instance, turpentine, its transparency is restored. We

have thus direct proof that transparency to light is due to molecular

condition. This may be most strikingly shown by an interesting

experiment of Sir David Brewster’s:--

If a glass tube is filled with nitrous acid vapour, which is of a dull

red colour, it admits freely the passage of the red and orange rays

with some of the others, and, if held upright in the sunshine, casts

a red shadow on the ground; by gently warming it with a spirit-lamp,

whilst in this position, it acquires a much deeper and blacker colour,

and becomes almost impervious to any of the rays of light; but upon

cooling it again recovers its transparency.

It has also been stated by the same exact experimentalist, that having

brought a purple glass to a red heat, its transparency was improved, so

that it transmitted green, yellow, and red rays, which it previously

absorbed; but the glass recovered its absorptive powers as it cooled.

A piece of yellowish-green glass lost its transparency almost entirely

by being heated. Native yellow orpiment becomes blood-red upon being

warmed, when nearly all but the red rays are absorbed; and pure

phosphorus, which is of a pale yellow colour, and transmits freely all

the coloured rays upon being melted, becomes very dark, and transmits

no light.

Chemistry affords numerous examples of a very slight change of

condition, producing absolute opacity in fluids which were previously

diaphanous.[88]

Charcoal absorbs all the light which falls upon it, but in some

of its states of combination, and in the diamond, which is pure

carbon, it is highly transparent. Gold and silver beaten into thin

leaves are permeated by the green and blue rays, and the metals in

combination with acids are all of them more or less transparent. What

becomes of the light which falls upon and is absorbed by bodies,

is a question which we cannot yet, notwithstanding the extensive

observations that have been made by some of the most gifted of men,

answer satisfactorily. In all probability, as already stated, it

is permanently retained within their substances; and many of the

experiments of exciting light in bodies when in perfect darkness, by

the electric spark and other means, appear to support the idea of light

becoming latent or hidden.

No body is absolutely transparent; some light is lost in passing even

through ethereal space, and still more in traversing our atmosphere.

Amongst the most curious instances of absorption is that which is

uniformly discovered in the solar spectrum, particularly when we

examine it with a telescope. We then find that the coloured rays are

crossed by a great number of dark bands or lines, giving no light;

these are generally called Fraunhofer’s dark lines, as it was to the

indefatigable exertions of that experimentalist, and by the aid of his

beautiful instruments, that most of them were discovered and measured,

and enumerated, although they were previously noticed by Dr. Wollaston.

It is quite clear that those lines represent rays which have been

absorbed in their passage from the sun to the earth: although some

of them have no doubt undergone absorption within the limits of the

earth’s atmosphere, we have every reason to believe, with Sir John

Herschel, that the principal absorption takes place in the atmosphere

of the sun.[89]

It has been proved by Dr. Miller, that the number of those dark

lines is continually varying with the alteration of atmospheric

conditions;[90] and the evidences which have been afforded, of peculiar

states of absorption by the gaseous envelope of the earth,--during the

prosecution of investigations on the chemical agencies of the sun’s

rays,--are of a sufficiently convincing character.

It has been calculated by Bouguer, that if our atmosphere, in its

purest state, could be extended rather more than 700 miles from the

earth’s surface instead of nearly 40, as it is at present, the sun’s

rays could not penetrate it, and this globe would roll on in darkness

and silence, without a vestige of vegetable form or of animal life. In

the Hebrew version of the Mosaic History, the reading is, “Let light

appear:” may not this really mean that the earth’s atmosphere was so

cleared of obstructing vapours, that the solar rays were enabled to

reach the earth? The same calculation supposes that sea-water loses

all its transparency at the depth of 730 feet; but a dim twilight must

prevail much deeper in the ocean.

The researches of Professor Edward Forbes have proved, that at the

depth of 230 fathoms in the Ægean sea, the few shelled animals that

exist are colourless: no plants are found within that zone; and that

industrious naturalist fixes the zero of animal life of those waters at

about 300 fathoms.[91] Since these zones mark the rapidly diminishing

light, it is evident that where life ceases to be must be beyond the

limits to which life can penetrate.

Our atmosphere, charged with aqueous vapour, serves to shield us from

the intense action of the solar powers. By it we are protected from

the destructive influences of the sun’s light and heat; enjoy those

modified conditions which are most conducive to the healthful being of

organic forms; to it we owe “the blue sky bending over all,” and those

beauties of morning and evening twilight of which

---- Sound and motion own the potent sway.

Responding to the charm with its own mystery.

To defective transparency, or rather to the different degrees of it, we

must attribute, in part, the colours of permeable media. Thus, a glass

or fluid appears yellow to the eye, because it has the property of

admitting the permeation of a larger quantity of the yellow rays than

of any others;--red, because the red rays pass it with the greatest

freedom; and so on for every other colour. In most cases the powers of

transmission and of reflection are similar; but it is not so in all; a

variety of fluor spar, which, while it transmits green light, reflects

blue, and the precious opal, are striking instances to the contrary.

Some glasses, which transmit yellow light have the singular power of

dispersing blue rays from one surface; and a solution of quinine in

water acidulated with sulphuric acid, although perfectly transparent

and colourless when held between the eye and the light, exhibits, if

viewed in a particular direction, a lively cerulean tint. These effects

being supposed to be due to the conditions of the surface, have been

called _epipolic_ phenomena.[92]

The careful investigation of these phenomena has made us acquainted

with some very interesting facts, and indeed discovered to us a set

of luminous rays which were previously unknown. The dispersion of

blue light from the surface of some yellow glasses--such as have been

coloured by the oxide of silver--is of a different order from that

which takes place with the solution of sulphate of quinine, or with

the fluor spar. The first depends upon a peculiar condition of the

surface, while the latter phenomena are due to a dispersion which

takes place _within_ the solid or fluid. In addition to the sulphate

of quinine, and the fluor spar, we obtain the same results in a very

marked manner by a canary yellow glass, coloured with the oxide of

uranium, and by a decoction of the inner bark of the horse-chesnut

tree. Mr. Stokes, who has investigated this class of phenomena, and

proposes to call it _Fluorescence_, from its being naturally seen in

fluor-spar, has shown that the peculiar internal dispersion, and the

consequent alteration of the colour of the ray, is due to an alteration

in its refrangibility. Whether this hypothesis prove to be the correct

one or not, it is certain that there exists a set of rays of far higher

refrangibility than those seen in the ordinary Newtonian spectrum. This

may be shown in the following manner: taking either of the solutions

named, or a block of uranium glass, throw upon one face, by means of

a prism, a very pure spectrum. On looking _into_ the glass or fluid

there will be seen, commencing amidst the most refrangible rays, a

new set of spectral rays, struggling to make their way through the

absorbent medium. These are of a blue colour in the quinine or chesnut

solution, and green in the uranium glass, and are seen extending

themselves far beyond the most refrangible rays of the ordinary

Newtonian spectrum. This is the space over which those rays which

have the power of producing chemical changes, such as are rendered

familiar by the practice of Photography, are detected in their greatest

activity. It has, therefore, been supposed that these fluorescent rays

are the chemical rays rendered luminous by the alteration of their

refrangibility. This view has received much support from the fact that

the extra spectral rays are crossed with numerous dark lines, and that

in the chemical impressions these lines are marked by unchanged spaces

which exactly coincide with them. There is, however, much doubt of the

correctness of this, since, in the uranium glass of such a thickness

that these visible rays are quite absorbed, the chemical rays still

pass.

However, the whole question requires, and is receiving, the most

searching investigation. The discovery of these phenomena, which are

included under the term of Fluorescence, is of that interesting and

important character, that it must be ranked as the most decided advance

which has been made in physical optics since the days of Newton.

It is not improbable that those rays of such high refrangibility may,

although they are under ordinary circumstances invisible to the human

eye, be adapted to produce the necessary degree of excitement upon

which vision depends in the optic nerves of the night-roaming animals.

The bat, the owl, and the cat, may see in the gloom of night by the aid

of rays which are invisible to, or inactive on the eyes of man, or of

those animals which require the light of day for perfect vision.

It is a general law of the radiant forces, that whenever they fall upon

any surface, a portion is thrown back or reflected at the same time

as other portions are absorbed or transmitted. Upon this peculiarity

appear to depend the phenomena of natural colour in bodies.

The white light of the sun is well known to be composed of several

coloured rays. Or rather, according to the theory of undulations, when

the rate at which a ray vibrates is altered, a different sensation

is produced upon the optic nerve. The analytical examination of

this question shows, that to produce a red colour the ray of light

must give 37,640 undulations in an inch, and 458,000000,000000 in

a second. Yellow light requires 44,000 undulations in an inch, and

535,000000,000000 in a second; whilst the effect of blue results from

51,110 undulations within an inch, and 622,000000,000000 of waves in

a second of time.[93] The determination of such points as these is

among the highest refinements of science, and, when contrasted with the

most sublime efforts of the imagination, they must appear immeasurably

superior.

If a body sends back white light unchanged, it appears white; if the

surface has the property of altering the vibration to that degree which

is calculated to produce redness, the result is a red colour: the

annihilation of the undulations produces blackness. By the other view,

or the corpuscular hypothesis, the beam of white light is supposed to

consist of certain coloured rays, each of which has physical properties

peculiar to itself, and thus is capable of producing different

physiological effects. These rays falling upon a transparent or an

opaque body suffer more or less absorption, and being thus dissevered,

we have the effect of colour. A red body absorbs all the rays but the

red; a blue surface, all but the blue; a yellow, all but the yellow;

and a black surface absorbs the whole of the light which falls upon it.

That natural colours are the result of white light, and not innate

properties of the bodies themselves, is most conclusively shown by

placing coloured bodies in monochromatic light of another kind, when

they will appear either of the colour of that light, or, by absorbing

it, become black; whereas, when placed in light of their own character,

the intensity of colour is greatly increasing.

Every surface has, therefore, a peculiar constitution, by which it

gives rise to the diversified hues of nature. The rich and lively

green, which so abundantly overspreads the surface of the earth, the

varied colours of the flowers, and the numberless tints of animals,

together with all those of the productions of the mineral kingdom,

and of the artificial combinations of chemical manufacture, result

from powers by which the relations of matter to light are rendered

permanent, until its physical conditions undergo some change.

There is a remarkable correspondence between the geographical position

of a region and the colours of its plants and animals. Within the

tropics, where

“The sun shines for ever unchangeably bright,”

the darkest green prevails over the leaves of plants; the flowers

and fruits are tinctured with colours of the deepest dye, whilst the

plumage of the birds is of the most variegated description and of the

richest hues. In the people also of these climes there is manifested

a desire for the most striking colours, and their dresses have all

a distinguishing character, not of shape merely, but of chromatic

arrangement. In the temperate climates everything is of a more subdued

variety: the flowers are less bright of hue; the prevailing tint of the

winged tribes is a russet brown; and the dresses of the inhabitants of

these regions are of a sombre character. In the colder portions of the

earth there is but little colour; the flowers are generally white or

yellow, and the animals exhibit no other contrast than that which white

and black afford. A chromatic scale might be formed, its maximum point

being at the equator, and its minimum at the poles.[94]

The influence of light on the colours of organized creation is well

shown in the sea. Near the shores we find sea-weeds of the most

beautiful hues, particularly on the rocks which are left dry by the

tides; and the rich tints of the actiniæ, which inhabit shallow water,

must have been often observed. The fishes which swim near the surface

are also distinguished by the variety of their colours, whereas those

which live at greater depths are grey, brown, or black. It has been

found that after a certain depth, where the quantity of light is so

reduced that a mere twilight prevails, the inhabitants of the ocean

become nearly colourless. That the sun’s ray alone gives to plants the

property of reflecting colour is proved by the process of blanching, or

_etiolation_, produced by artificially excluding the light.

By a triangular piece of glass--a prism,--we are enabled to resolve

light into its ultimate rays. The white pencil of light which falls

on the first surface of the prism is bent from its path, and coloured

bands of different colours are obtained. These bands or rays observe a

curious constancy in their positions: the red ray is always the least

bent out of the straight path: the yellow class comes next in the

order of refrangibility; and the blue are the most diverted from the

vertex of the prism. The largest amount of illuminating power exists

in the yellow ray, and it diminishes towards either end.[95] It is not

uninteresting to observe something like the same variety of colour

occurring at each end of the prismatic spectrum. The strict order

in which the pure and mixed coloured rays present themselves is as

follows:--

1. The _extreme red_: a ray which can only be discovered when the eye

is protected from the glare of the other rays by a cobalt blue glass,

is of a crimson character--a mixture of the _red_ and the _blue_, red

predominating.[96]

2. The _red_: the first ray visible under ordinary circumstances.

3. The _orange_: red passing into and combining with yellow.

4. The _yellow_: the most intensely luminous of the rays.

5. The _green_: the yellow passing into and blending with the blue.

6. The _blue_: in which the light very rapidly diminishes.

7. The _indigo_: the dark intensity of blue.

8. The _violet_: the _blue_ mingled again with the _red_--blue being in

excess.

9. The _lavender grey_: a neutral tint, produced by the combination of

the red, blue, and yellow rays, which is discovered most easily when

the spectrum is thrown upon a sheet of turmeric paper.

10. The fluorescent rays: which are either a _pure silvery blue_ or a

delicate _green_.

Newton regarded the spectrum as consisting of seven colours of

definite and unvarying refrangibility. Brewster and others appear to

have detected a great diffusion of the colours over the spectrum,

and regard white light as consisting only of three rays, which in the

prismatic images overlap each other; and from these--red, yellow,

and blue--all the others can be formed by combination in varying

proportions. The truth will probably be found to be, that the ordinary

prismatic spectrum is a compound of two spectra:--that is, as we have

the ordinary rainbow, and a supplementary bow, the colours of which are

inverted, so the extraordinary may be somewhat masked by the intense

light of the ordinary spectrum; and yet by overlapping produce the

variations of colour in the rays. We have already examined the heating

power found in these coloured bands, which, although shown to be in a

remarkable manner in constant agreement with the colour of a particular

ray, is not directly connected with it; that is, not as the effect of a

cause, or the contrary. The chemical action of the solar rays, to which

from its important bearings we shall devote a separate chapter, has, in

like manner with heat, been confounded with the sun’s luminous power;

but although associated with light and heat, and modified by their

presence, it must be distinguished from them.

We find the maximum of heat at one end of the spectrum, and that of

chemical excitation at the other--luminous power observing a mean point

between them. Without doubt we have these powers acting reciprocally,

modifying all the phenomena of each other, and thus giving rise to the

difficulties which beset the inquirer on every side.

We have beautiful natural illustrations of luminous refraction in

the rainbow and in the halo: in both cases the rays of light being

separated by the refractive power of the falling rain drop, or the

vesicles which form the moisture constituting a fog. In the simple toy

of the child--the soap-bubble floating upon the air--the philosopher

finds subjects for his contemplation; and from the unrivalled play of

colours which he discovers in that attenuated film, he learns that the

varying thicknesses of surfaces influence, in a most remarkable manner,

the colours of the sunbeam. Films of oil floating upon water present

similar appearances; and the colours developed in tempering steel

are due entirely to the thickness of the oxidized surface produced

by heat. There have lately been introduced some beautiful specimens

of paper rendered richly iridescent by the following process:--A

solution of a gum resin in chloroform is floated upon water, where

it forms a film giving all the colours of Newton’s rings. A sheet of

paper which has been previously sunk in the water is carefully lifted,

and the film thus removed adheres with great firmness to the paper,

and produces this rich and curious play of colour. The rich tints

upon mother-of-pearl, in the feathers of many birds, the rings seen

in the cracks of rock-crystal, or between the unequal faces of two

pieces of glass, and produced by many chemical and indeed mechanical

operations--are all owing to the same cause;--the refraction of the

luminous pencil by the condition of the film or surface. If we take

one of those steel ornaments which are formed by being covered with

an immense number of fine lines, it will be evident that these striæ

present many different angles of reflection, and that, consequently,

the rays thrown back will, at some point or another, have a tendency

to cross each other. The result of this is, that the quantity of

light is augmented at some points of intersection, and annihilated at

others.[97] Out of the investigation of the phenomena of diffraction,

of the effects of thin and thick plates upon light, and the results of

interference, has arisen the discovery of one of the most remarkable

conditions within the range of physical science.

_Two bright lights may be made to produce darkness._--If two pencils

of light radiate from two spots very close to each other in such a

manner that they cross each other at a given point, any object placed

at that line of interference will be illuminated with the sum of the

two luminous pencils. If we suppose those rays to move in waves, and

the elevation of the wave to represent the maximum of luminous effect,

then the two waves meeting, when they are both at the height of their

undulation, will necessarily produce a spot of greater intensity. If

now we so arrange the points of radiation, that the systems of luminous

waves proceed irregularly, and that one arrives at the screen half an

undulation before the other, the one in elevation falling into the

depression of the other, a mutual annihilation is the consequence. This

fact, paradoxical as it may appear, was broadly stated by Grimaldi,

in the description of his experiments on the inflection of light, and

has been observed by many others. The vibratory hypothesis, seizing

upon the analogy presented by two systems of waves in water, explains

this plausibly, and many similar phenomena of what is called the

_interference of light_; but still upon examination it does not appear

that the explanation is quite free from objection.[98]

Another theory, not altogether new to us, it being indicated in Mayer’s

hypothesis of three primary colours (1775), and to be found as a

problem in some of the Encyclopædias of the last century, has been put

forth, in a very original manner, by that master-mind of intellectual

Germany, Goethe; and from the very comprehensive views which this

poet-philosopher has taken of both animal and vegetable physiology

(views which have been adopted by some of the first naturalists of

Europe), we are bound to receive his theory of colours with every

respect and attention.

Goethe regards colour as the “thinning” of light; for example, by

obstructing a portion of white light, yellow is produced; by reducing

it still farther, red is supposed to result; and by yet farther

retarding the free passage of the beam, we procure a blue colour, which

is the next remove from blackness, or the absence of light. There is

truth in this; it bears about it a simplicity which will satisfy many

minds; by it many of the phenomena of colour may be explained: but it

is insufficient for any interpretation of several of those laws to

which the other theories do give us some insight.

Newton may have allowed himself to be misled by the analogy presented

between the seven rays of the spectrum and the notes in an octave.

The mystic number, seven, may have clung like a fibre of the web of

superstition to the cloak of the great philosopher; but the attack made

by Goethe upon the Newtonian philosophy betrays the melancholy fact of

his being diseased with the lamentable weakness of too many exalted

minds--an overweening self-esteem.

The polarization of light, as it has been unfortunately

called--unfortunately, as conveying an idea of determinate and

different points or poles, which only exists in hypothetical

analogy--presents to us a class of phenomena which promise to unclose

the mysterious doors of the molecular constitution of bodies.

This remarkable condition, as produced by the reflection of light from

glass at a particular angle, was first observed by Malus, in 1808,[99]

when amusing himself by looking at the beams of the setting sun,

reflected from the windows of the Luxembourg Palace through a double

refracting prism. He observed that when the prism was in one position,

the windows with their golden rays were visible; but that turned

round a quarter of a circle from that position, the reflected rays

disappeared although the windows were still seen.

The phenomenon of double refraction was noticed, in the first instance,

by Erasmus Bartholin, in Iceland-spar, a crystal the primary form of

which is a rhombohedron; who perceived that the two images produced by

this body were not in the same physical conditions.[100] It was also

studied by Huyghens and Sir Isaac Newton, and to our countryman we owe

the singular idea that a ray of light emerging from such a crystal

has _sides_. This breaking up of the beam of light into two,--which

is shown by looking through a pin-hole on a card through a crystal of

Iceland spar, when two holes become visible, is due to the different

states of tension in which the different layers constituting the

crystal exist.

In thus separating the ray of light into two rays, the condition

called polarisation has been produced, and by experiment we discover

that the single ray has properties different from those of the compound

or ordinary ray.

It is somewhat difficult to explain what is meant by, and what are the

conditions of, _polarised light_. In the first instance let us see by

what methods this peculiar state may be brought about.

If we reflect a ray of light from the surface of any body, fluid or

solid, but not metallic, at an angle between 53° and 68° it undergoes

what has been called _plane polarisation_. It may also be produced by

the refraction of light from several refracting surfaces acting upon

the pencil of light in succession; as by a bundle of plates of glass.

Each surface polarises a portion of the pencil, and the number of

plates necessary to polarise a whole beam depends upon the intensity of

the beam and the angle of incidence. Thus, the light of a wax candle

is wholly polarised by forty-seven plates of glass at an angle of 40°

41'; while at an angle of 79° 11' it is polarised by eight plates.

Again, plane polarisation may be produced by the double refraction of

crystals. Each of the two pencils is polarised, like light reflected

from glass at an angle of 56° 45', but in opposite planes.

Non-scientific readers will still ask,--What is this mysterious

condition of light which is produced by reflection and refraction at

peculiar angles to the incident ray. It is one of the most difficult of

problems to express in popular language. The conditions are, however,

these:--

An ordinary ray of light will be reflected from a reflecting surface at

whatever angle that surface may be placed in relation to the incident

beam.

A polarised ray of light is not reflected in all positions of the

reflecting surface.

An ordinary ray of light is freely transmitted through a transparent

medium, as glass, in whatever position it may be placed relative to the

source of light.

A polarised ray of light is not transmitted in all the positions of the

permeable medium.

Supposing a plate of glass is presented at the angle 56° to a polarised

ray, and the plane of incidence or reflexion is at right angles to the

plane of polarisation of the ray, _no light is reflected_. If we turn

the plate of glass round through 90°, when the plane of reflexion is

parallel to that of polarisation _the light is reflected_. If we turn

the plate round another 90°, so that the plane of reflexion and of

polarisation are parallel to each other, again _no light is reflected_;

and if we turn it through another 90° the reflection of the ray again

takes place.

Precisely the same result takes place when, instead of being reflected,

the polarised ray is transmitted.

Some substances have peculiar polarizing powers: _the tourmaline_ is a

familiar example. If a slice of tourmaline is taken, and we look at a

common pencil of light through it, we see it in whatever position we

may place the transparent medium. If, however, we look at a pencil of

polarised light, and turn the crystal round, it will be found that in

two positions the light is stopped, and that in two other positions it

passes freely through it to the eye.

By way of endeavouring to conceive something of what may be the

conditions which determine this very mysterious state, let us suppose

each ray of light to vibrate in two planes at right angles to each

other: one wave being vertical and the other horizontal. We have many

examples of this compound motion. The mast of a ship, by the force with

which she is urged through the water, describes a vertical wave, while

by the roll of the billows across which she sails, a lateral undulation

is produced at the same time. We may sometimes observe the same thing

when a field of corn is agitated by a shifting wind on a gusty day.

The hypothesis therefore is, that every ray of ordinary light consists

of two rays vibrating in different planes; and that these rays,

separated one from the other, have the physical conditions which we

call _polarized_.

The most transparent bodies may be regarded as being made up of atoms

arranged in certain planes. Suppose the plane of lamination of any

substance to be vertical in position, it would appear that the ray

which has a vertical motion passes it freely, whereas if we turn the

body round so that the planes of lamination are at right angles to the

plane of vibration of the ray, it cannot pass.

That some action similar to that which it is here endeavoured to

express in popular language does take place, is proved by the

correctness of the results deduced by rigid mathematical analyses

founded on this hypothesis.

There are two other conditions of the polarization of light--called

_circular_ and _elliptical_ polarization. The first is produced by

light when it is twice reflected from the second surface of bodies at

their angle of maximum polarization, and the second by reflexions from

the surfaces of metals at angles varying from 70° 45' to 78° 30'. The

motion of the wave in the first is supposed to be circular, or to be

that which is represented by looking along the centre of a corkscrew

as it is turned round. At every turn of the medium effecting _circular

polarization_ the colour of the ray of light is changed after a uniform

order. If turned in one direction, they change through red, orange,

yellow, green, and violet; and if in the other direction, the colours

appear in the contrary order.

The variety of striking effects produced by the polarization of light;

the unexpected results which have sprung from the investigation of the

laws by which it is regulated; and the singular beauty of many of its

phenomena, have made it one of the most attractive subjects of modern

science.

Ordinary light passes through transparent bodies without producing any

very striking effects in its passage; but this _extraordinary_ beam

of light has the power of insinuating itself between the molecules

of bodies, and by illuminating them, and giving them every variety

of prismatic hue, of enabling the eye to detect something of the

structure of the mass. The chromatic phenomena of polarized light are

so striking, that no description can convey an adequate idea of their

character.

Spectra more beautiful and intense than the prismatic image,--systems

of rings far excelling those of thin plates,--and forms of the most

symmetric order, are constantly presenting themselves, as the polarized

ray is passed through various transparent substances; the path of the

ray indicating whether the crystal has been formed round a single

nucleus or axis, or whether it has been produced by aggregation

around two axes. The coloured rings, and the dark or luminous crosses

which distinguish the path of the polarized ray, are respectively

due to different states of tension amongst the particles, although

those differences are so slight, that no other means is of sufficient

delicacy to detect the variation.

The poetry which surrounds these, in every way, mysterious conditions

of the solar beam, is such, that it is with difficulty that imagination

is restrained by the stern features of truth. The uses of this peculiar

property in great natural phenomena are not yet made known to us; but,

since we find on every side of us the natural conditions for thus

separating the beam of light, and effecting its polarization, there

must certainly be some most important end for which it is designed by

Him who said, “Let there be Light.”

It must not be forgotten that we have at command the means of showing

that the chromatic phenomena of polarized light are due to atomic

arrangement. By altering the molecular arrangement of transparent

bodies, either by heat or by mere mechanical pressure, the unequal

tension or strain of the particles is at once indicated by means of

the polarized ray of light and its rings of colour. Differences in the

chemical constitution of bodies, too slight to be discovered by any

other mode of analysis, can be most readily and certainly detected by

this luminous investigator of the molecular forces.[101]

Although we cannot enter into an examination of all the conditions

involved in the polarization of, and the action of matter on, ordinary

light, it will be readily conceived, from what has been already stated,

that some most important properties are indicated, beyond those which

science has made known.

Almost every substance in nature, in some definite position, appears

to have the power of producing this change upon the solar ray, as

may be satisfactorily shown by examining them with a polarizing

apparatus.[102] The sky at all times furnishes polarized light, which

is most intense where it is blue and unclouded, and the point of

maximum polarization is varied according to the relative position of

the sun and the observer. A knowledge of this fact has led to the

construction of a “Solar Clock,”[103] with which the hour can be

readily determined by examining the polarized condition of the sky.

It has been stated, that chemical change on the Daguerreotype plates

and on photographic papers is more readily produced by the polarized

than by the ordinary sunbeam.[104] If this fact be established by

future investigations, we advance a step towards the discovery so much

desiderated of the part it plays in natural operations.

The refined and accurate investigations of Dr. Faraday stand

prominently forward amid those which will redeem the present age from

the charge of being superficial, and they will, through all time, be

referred to as illustrious examples of the influence of a love of truth

for truth’s sake, in entire independence of the marketable value, which

it has been unfortunately too much the fashion to regard. The searching

examination made by this “interpreter of nature” into the phenomena

of electricity in all its forms, has led him onward to trace what

connexion, if any, existed between this great natural agent and the

luminous principle.

By employing that subtile analyzer, a polarized ray, Dr. Faraday

has been enabled to detect and exhibit effects of a most startling

character. He has proved magnetism to have the power of influencing a

ray of light in its passage through transparent bodies. A polarized ray

is passed through a piece of glass or a crystal, or along the length

of a tube filled with some transparent fluid, and the line of its path

carefully observed; if, when this is done, the solid or fluid body is

brought under powerful magnetic influence, such as we have at command

by making a very energetic voltaic current circulate around a bar of

soft iron, it will be found that the polarized light is disturbed;

that, indeed, it does not permeate the medium along the same line.[105]

This effect is most strikingly shown in bodies of the greatest density,

and diminished in fluids, the particles of which are easily moveable

over each other, and has not hitherto been observed in any gaseous

medium. The question, therefore, arises,--does magnetism act directly

upon the ray of light, or only indirectly, by producing a molecular

change in the body through which the ray is passing? This question,

so important in its bearings upon the connexion between the great

physical powers, will, no doubt, before long receive a satisfactory

reply. A medium is necessary to the production of the result, and, as

the density of the medium increases, the effect is enlarged: it would

therefore appear to be due to a disturbance by magnetic force of the

particles which constitute the medium employed.

Without any desire to generalize too hastily, we cannot but express

a feeling,--amounting to a certainty in our own mind,--that those

manifestations of luminous power, connected with the phenomena of

terrestrial magnetism, which are so evident in all the circumstances

attendant upon the exhibition of Aurora Borealis, and those luminous

clouds which are often seen, independent of the Northern Lights, that

a very intimate, relation exists between the solar radiations and that

power which so strangely gives polarity to this globe of ours.

In connexion with the mysterious subject of solar light, it is

important that we should occupy a brief space in these pages with the

phenomena of vision, which is so directly dependent upon luminous

radiation.

The human eye has been rightly called the “masterpiece of divine

mechanism;” its structure is complicated, yet all the adjustments of

its parts are as simple as they are perfect. The eye-ball consists of

four coats. The cornea is the transparent coat in front of the globe;

it is the first optical surface, and this is attached to the sclerotic

membrane, filling up the circular aperture in the white of the eye;

the choroid coat is a very delicate membrane, lining the sclerotic,

and covered with a perfectly black pigment on the inside; and close to

this lies the most delicately reticulated membrane, the retina, which

is, indeed, an extension of the optic nerve. These coats enclose three

humours,--the aqueous, the vitreous, and the crystalline humours.

The eye, in its more superficial mechanical arrangements, presents

exactly the same character as a camera obscura, the cornea and

crystalline lens receiving the images of objects refracting and

inverting them; but how infinitely more beautiful are all the

arrangements of the organ of vision than the dark chamber of Baptista

Porta![106] The humours of the eye are for the purpose of correcting

the aberrations of light, which are so evident in ordinary lenses,

and for giving to the whole an achromatic character. Both spherical

and chromatic aberration are corrected, the latter not entirely, and

by the agency of the cornea and the crystalline lens perfect images

are depicted on the retina, in a similar way to those very charming

pictures which present themselves in the table of the camera obscura.

The seat of vision has been generally supposed to be the retina;

but Mariotte has shown that the base of the optic nerve, which is

immediately connected with the retina, is incapable of conveying an

impression to the brain. The choroid coat, which lies immediately

behind the retina, is regarded by Mariotte and Bernoulli as the more

probable seat of vision. The retina, being transparent, offers no

obstruction to the passage of the light onward to the black surface of

the choroid coat, from which the vibrations are, in all probability,

communicated to the retina and conveyed to the brain. Howbeit, upon one

or the other of these delicate coats a distinct image is impressed

by light, and the communication made with the brain possibly by a

vibratory action. We may trace up the phenomena of vision to this

point; we may conceive undulations of light, differing in velocity and

length of wave, occasioning corresponding tremors in the neuralgic

system of the eye; but how these vibrations are to communicate

correct impressions of length, breadth, and thickness, no one has yet

undertaken to explain.

It has, however, been justly said by Herschel:--

“It is the boast of science to have been able to trace so far the

refined contrivances of this most admirable organ, not its shame to

find something still concealed from scrutiny; for, however anatomists

may differ on points of structure, or physiologists dispute on modes

of action, there is that in what we _do_ understand of the formation

of the eye, so similar, and yet so infinitely superior to a product

of human ingenuity; such thought, such care, such refinement, such

advantage taken of the properties of natural agents used as mere

instruments for accomplishing a given end, as force upon us a

conviction of deliberate choice and premeditated design, more strongly,

perhaps, than any single contrivance to be found whether in art or

nature, and renders its study an object of the greatest interest.”[107]

Has the reader ever asked himself why it is, having two eyes, and

consequently two pictures produced upon the tablets of vision, that we

see only one object? According to the law of visible direction, all the

rays passing through the crystalline lenses converge to one point upon

the retina,--and as the two images are coincident and nearly identical,

they can only produce the sensation of one upon the brain.

When we look at any round object, as the ornamented moderator lamp

before us, first with one eye, and then with the other, we discover

that, with the right eye, we see most of the right-hand side of the

lamp, and with the left eye more of the left-hand side. These two

images are combined, and we see an object which we know to be round.

This is illustrated in a most interesting manner by the little optical

instrument, _the Stereoscope_. It consists either of two mirrors placed

each at an angle of 45°, or of two semi-lenses turned with their curved

sides towards each other. To view its phenomena, two pictures are

obtained by the camera obscura on photographic paper of any object in

two positions, corresponding with the conditions of viewing it with the

two eyes. By the mirrors or the lenses these dissimilar pictures are

combined within the eye, and the vision of an actually solid object is

produced from the pictures represented on a plane surface. Hence the

name of the instrument; which signifies, _Solid I see_.

Analogy is often of great value in indicating the direction in which to

seek for a truth; but analogical evidence, unless where the resemblance

is very striking, should be received with caution. Mankind are so ready

to leap to conclusions without the labour necessary for a faithful

elucidation of the truth, that too often a few points of resemblance

are seized upon, and an inference is drawn which is calculated to

mislead.

There is an idea that the phenomena of sound bear a relation to those

of light,--that there exists a resemblance between the chromatic

and the diatonic scales. Sound, we know, is conveyed by the beating

of material particles--the air--upon the auditory membrane of the

ear, which have been set in motion by some distant disturbance of

the medium through which it passes. Light has been supposed to act

on the optic nerve in the same manner. If we imagine colour to be

the result of vibrations of different velocities and lengths, we can

understand that under some of these tremors, first established on the

nerves, and through them conveyed to the brain, sensations of pain

or pleasure may result, in the same way as sharp or subdued sounds

are disagreeable or otherwise. Intensely coloured bodies do make an

impression upon perfectly blind men; and those who, being born blind,

know no condition of light or colour, will point out a difference

between strongly illuminated red and yellow media. When the eyes are

closed we are sensible to luminous influence, and even to differences

of colour. We must consequently infer that light produces some peculiar

action upon the system of nerves in general; this may or may not

be independent of the chemical agency of the solar radiations; but

certainly the excitement is not owing to any calorific influence. The

system of nerves in the eye is more delicately organized, and of course

peculiarly adapted to all the necessities of vision.

Thus far some analogy does appear to exist between light and sound;

but the phenomena of the one are so much more refined than those of

the other--the impressions being all of them of a far more complicated

character, that we must not be led too far by the analogical evidence

in referring light, like sound, to mere material motion.

It was a beautiful idea that real impressions of external objects

are made upon the seat of vision, and that they are viewed, as in a

picture, by something behind the screen,--that these pictures become

dormant, but are capable of being revived by the operations of the mind

in peculiar conditions; but we can only regard it as a philosophical

speculation of a poetic character, the truth or falsehood of which we

are never likely to be enabled to establish.[108]

That which sees will never itself be visible. The secret principle

of sensation,--the mystery of the life that is in us,--will never be

unfolded to finite minds.

Numerous experiments have been made from time to time on the influence

of light upon animal life. It has been proved that the excitement of

the solar rays is too great for the healthful growth of young animals;

but, at the same time, it appears probable that the development of

the functional organs of animals requires, in some way, the influence

of the solar rays. This might, indeed, have been inferred from the

discovery that animal life ceases in situations from which light is

absolutely excluded. The instance of the Proteus of the Illyrian lakes

may appear against this conclusion. This remarkable creature is found

in the deep and dark recesses of the calcareous rocks of Adelsburg, at

Sittich; and it is stated, also in Sicily, and in the Mammoth caves

of Kentucky. Sir Humphry Davy describes the Proteus anguinus as “an

animal to whom the presence of light is not essential, and who can

live indifferently in air and in water, on the surface of the rock,

or in the depths of the mud.” The geological character of rocks,

however, renders it extremely probable that these animals may have

descended with the water, percolating through fissures from very near

the surface of the ground. All the facts with which science has made us

acquainted--and both natural and physical science has been labouring

with most untiring industry in the pursuit of truth--go to prove

that light is absolutely necessary to organization. It is possible

the influence of the solar radiations may extend beyond the powers

of the human senses to detect luminous or thermic action, and that

consequently a development of animal and vegetable forms may occur

where the human eye can detect no light; and under such conditions

the Proteus may be produced in its cavernous abodes, and also those

creatures which live buried deep in mud. Some further consideration of

the probable agency of light will occupy us, when we come to examine

the phenomena of vital forces.

Light is essentially necessary to vegetable life; and to it science

refers the powers which the plant possesses of separating carbon from

the air breathed by the leaves, and secreting it within its tissues for

the purpose of adding to its woody structure. As, however, we have, in

the growing plant, the action of several physical powers exerted to

different ends at the same time, the remarkable facts which connect

themselves with vegetable chemistry and physiology are deferred for a

separate examination.

The power of the solar rays to produce in bodies that peculiar gleaming

light which we call phosphorescence, and the curious conditions under

which this phenomenon is sometimes apparent, independent of the sun’s

direct influence, present a very remarkable chapter in the science of

luminous powers.

The phosphorescence of animals is amongst the most surprising of

nature’s phenomena, and it is not the less so from our almost entire

ignorance of the cause of it. Many very poetical fancies have been

applied in description of these luminous creations; and imagination

has found reason why they should be gifted with these extraordinary

powers. The glow-worm lights her lamp to lure her lover to her bower,

and the luminous animalcules of the ocean are employed in lighting up

the fathomless depths where the sun’s rays cannot penetrate, to aid its

monsters in their search for prey. “The lamp of love--the pharos--the

telegraph of the night,--which scintillates and marks, in the silence

of darkness, the spot appointed for the lover’s rendezvous,”[109] is

but a pretty fiction; for the glow-worm shines in its infant state,

in that of the larva, and when in its aurelian condition. Of the

dark depths of the ocean it may be safely affirmed that no organized

creation lives or moves in its grave-like silence to require this

fairy aid. Fiction has frequently borrowed her creations from science.

In these cases science appears to have made free with the rights of

fiction.

The glow-worms (_lampyris noctiluca_), it is well known, have the

power of emitting from their bodies a beautiful pale bluish-white

light, shining during the hours of night in the hedge-row, like crystal

spheres. It appears, from the observations of naturalists, that these

insects never exhibit their light without some motion of the body or

legs;--from this it would seem that the phosphorescence was dependent

upon nervous action, regulated at pleasure by the insect; for they

certainly have the power of obscuring it entirely. If the glow-worm is

crushed, and the hands or face are rubbed with it, luminous streaks,

similar to those produced by phosphorus, appear. They shine with

greatly increased brilliancy in oxygen gas and in nitrous oxide. From

these facts may we not infer that the process by which this luminosity

is produced, whatever it may be, has a strong resemblance to that of

respiration?

There are several varieties of flies, and three species of beetles of

the genus _Elater_, which have the power of emitting luminous rays.

The great lantern-fly of South America is one of the most brilliant, a

single insect giving sufficient light to enable a person to read. In

Surinam a very numerous class of these insects are found, which often

illuminate the air in a remarkable manner. In some of the bogs of

Ireland a worm exists which gives out a bright green light; and there

are many other kinds of creatures which, under certain circumstances,

become luminous in the dark. This is always dependent upon vitality;

for all these animals, when deprived of life, cease to shine.

At the same time we have many very curious instances of phosphorescence

in dead animal and vegetable matter; the lobster among the Crustacea,

and the whiting among fishes, are striking examples; decayed wood

also emits much light under certain conditions of the atmosphere.

This development of light does not appear to be at all dependent upon

putrefaction; indeed, as this process progresses, the luminosity

diminishes. We cannot but imagine that this light is owing, in the

first place, to direct absorption by, and fixation within, the

corpuscular structure of those bodies, and that it is developed by the

decomposition of the particles under the influence of our oxygenous

atmosphere.

The pale light emitted by phosphorus in the dark is well known; and

this is evidently only a species of slow combustion, a combination of

the phosphorus with the oxygen of the air. Where there is no oxygen,

phosphorus will not shine; its combustion in chlorine or iodine vapour

is a phenomenon of a totally different character from that which we are

now considering. This phosphorescence of animal and vegetable matter

has been regarded as something different from the slow combustion of

phosphorus; but, upon examination, all the chemical conditions are

found to be the same, and it is certainly due to a similar chemical

change.

The luminous matter of the dead whiting or the mackerel may be

separated by a solution of common salt or of sulphate of magnesia; by

concentrating these solutions the light disappears; but it is again

emitted when the fluid is diluted. The entire subject is, however,

involved in the mystery of ignorance, although it is a matter quite

within the scope of any industrious observer. The self-emitted light

of the carbuncle of the romancer is realized in these remarkable

phenomena.

The phosphorescence of some plants and flowers is not, perhaps, of

the same order as that which belongs to either of the conditions we

have been considering. It appears to be due rather to an absorption of

light and its subsequent liberation. If a nasturtium is plucked during

sunshine, and carried into a dark room, the eye, after it has reposed

for a short time, will discover the flower by a light emitted from its

leaves.

The following remarkable example, and an explanation of it by the poet

Goethe, is instructive:--

“On the 19th of June, 1799, late in the evening, when the twilight was

deepening into a clear night, as I was walking up and down the garden

with a friend, we very distinctly observed a flame-like appearance

near the oriental poppy, the flowers of which are remarkable for their

powerful red colour. We approached the place, and looked attentively

at the flowers, but could perceive nothing further, till at last, by

passing and repassing repeatedly, while we looked side-ways on them, we

succeeded in renewing the appearance as often as we pleased. It proved

to be a physiological phenomenon, and the apparent corruscation was

nothing but the spectrum of the flower in the complementary blue-green

colour. The twilight accounts for the eye being in a perfect state

of repose, and thus very susceptible, and the colour of the poppy is

sufficiently powerful in the summer twilight of the longest days to act

with full effect, and produce a complementary image.”[110]

The leaves of the _œnothera macrocarpa_ are said to exhibit phosphoric

light when the air is highly charged with electricity. The agarics

of the olive-grounds of Montpelier have been observed to be luminous

at night; but they are said to exhibit no light, even in darkness,

_during the day_. The subterranean passages of the coal mines near

Dresden are illuminated by the phosphorescent light of the _rhizomorpha

phosphoreus_, a peculiar fungus. On the leaves of the Pindoba palm, a

species of agaric grows which is exceedingly luminous at night; and

many varieties of the lichens, creeping along the roofs of caverns,

lend to them an air of enchantment by the soft and clear light which

they diffuse. In a small cave near Penryn, a luminous moss is abundant;

and it is also found in the mines of Hesse. According to Heinzmann, the

_rhizomorpha subterranea_ and _aidulæ_ are also phosphorescent.

It is but lately that a plant which abounds in the jungles in the

Madura district of the East Indies was sent to this country, which,

although dead, was remarkably phosphorescent; and, when in the

living state, the light which it emitted was extraordinarily vivid,

illuminating the ground for some distance. Those remarkable effects

may be due, in some cases, to the separation of phosphuretted hydrogen

from decomposing matter, and, in others, to some peculiar electric

manifestation.

The phosphorescence of the sea, or that condition called by fishermen

_brimy_, when the surface, being struck by an oar, or the paddle-wheels

of a steamer, gives out large quantities of light, has been attributed

to the presence of myriads of minute insects which have the power

of emitting light when irritated. The night-shining nereis (_Nereis

noctiluca_) emits a light of great brilliancy, as do several kinds of

the mollusca. The nereides attach themselves to the scales of fishes,

and thus frequently render them exceedingly luminous. Some of the

crustaceæ possess the same remarkable property;--twelve different

species of _cancer_ were taken up by the naturalists of the Zaire

in the Gulf of Guinea.[111] The _cancer fulgens_, discovered by Sir

Joseph Banks, is enabled to illuminate its whole body, and emits

vivid flashes of light. Many of the medusæ also exhibit powerful

phosphorescence.[112] These noctilucous creatures are, many of them,

exceedingly minute, several thousands being found in a tea-cup of sea

water. They float near the surface in countless myriads, and when

disturbed they give out brilliant scintillations, often leaving a train

of light behind them.[113] By microscopic examination no other fact has

been elicited than that these minute beings contain a fluid which, when

squeezed out, leaves a line of light upon the surface of water. The

appearance of these creatures is almost invariably on the eve of some

change of weather, which would lead us to suppose that their luminous

phenomena must be connected with electrical excitation; and of this,

the investigations of Mr. C. Peach, of Fowey, communicated to the

British Association at Birmingham, furnish the most satisfactory proofs

we have as yet obtained.

Benvenuto Cellini gave a curious account of a carbuncle which shone

with great brilliancy in the dark.[114] The same thing has been stated

of the diamond; but it appears to be necessary to procure these

emissions of light, that the minerals should be first warmed near a

fire. From this it may be inferred that the luminous appearance is

of a similar character to that of fluor spar, and of numerous other

earthy minerals, which, when exposed to heat, phosphoresce with great

brilliancy. Phosphorescent glow can also be excited in similar bodies

by electricity, as was first pointed out by Father Beccaria, and

confirmed by Mr. Pearsall.[115] These effects, it must be remembered,

are distinct from the electric spark manifested upon breaking white

sugar in the dark, or scratching sulphuret of zinc.

In the instances adduced there is not necessarily any exposure to the

sunshine required. It is probable that two, if not three, distinct

phenomena are concerned in the cases above quoted, and that all of them

are distinct from animal phosphorescence, or the luminous appearance

of vegetables. They, however, certainly prove, either that light is

capable of becoming latent, or that it is only a condition of matter,

in which it may be made manifest by any disturbance of the molecular

forces. We have, in answer to this, very distinct evidence that

some bodies do derive this property from the solar rays. Canton’s

phosphorus, which is a sulphuret of calcium, will, having been exposed

to the sun, continue luminous for some time after it is carried into

the dark; as will also the Bolognian stone,--a sulphuret of barium.

This result appears to be due to a particular class of the solar rays;

for it has been found, if these sulphurets, spread smoothly on paper,

are exposed to the influence of the solar spectrum for some little

time, and then examined in the dark, that luminous spaces appear,

exactly corresponding with the most refrangible rays, or those which

excite chemical change; and one very remarkable fact must not be

forgotten--the dark rays of the spectrum beyond the violet produce a

lively phosphorescence, which is _extinguished_ by the action of the

rays of least refrangibility, or the heat rays--whilst artificial heat,

such as a warm iron, produces a very considerable elevation of the

phosphorescent effect.[116] It is not improbable, that the fluorescent

rays of Mr. Stokes may be materially concerned in producing the

phenomena of phosphorescence: experiments are, however, required to

prove this.

In these allied phenomena we have effects which are evidently dependent

upon several dissimilar causes. The phosphorescence of the living

animal is due, without doubt, to nervous excitation: that of the living

vegetable to solar luminous influence; and in the case of the mosses of

caverns, &c. to the chemical agency of the sun’s rays, which appears to

be capable of conduction. In the dead organic matter we have a purely

chemical action developing the light, and in the inorganic bodies we

have peculiar molecular constitution, by which an absorption of light

appears to take place.

The subject is one of the greatest difficulty; the torch of science

is too dim to enable us to see the causes at work in producing these

marvellous effects. The investigation leads, to a certain extent, to

the elucidation of many of the secrets of luminous action; and the

determination of the question, whether light is an emanation from the

sun, or only a subtile principle diffused through all matter, which is

excited by solar influence, is intimately connected with the inquiry.

It has been stated that matter is necessary to the development of

light; that no luminous effect would be produced if it were not for

the presence of matter. Of this we not only have no proof, but such

evidence as we have is against the position. There is no loss of light

in the most perfect vacuum we can produce by any artificial means,

which should be the case if matter was concerned in the phenomena of

light, as a cause.

Colour is certainly a property regulated by material bodies; or

rather, the presence of matter is necessary to the production of

colour. Chlorine gas is a pale yellow, and nitrous vapour a yellowish

red. These and one or two other vapours, which are near the point of

condensation into fluids, are the only coloured gaseous or vaporiform

bodies. The sky is blue, because the material particles of the

atmosphere reflect back the blue rays. But we have more practical

illustrations than this. The flame of hydrogen burning with oxygen

gives scarcely any light; allow it to impinge on lime, a portion of

which is carried off by the heat of the flame, and the most intense

artificial light with which we are acquainted is produced. Hydrogen gas

alone gives a flame in which nearly all but the blue rays are wanting:

place a brush of steel or asbestos in it, and many of the other rays

are at once produced. An argand lamp, and more particularly the lamp

in which camphine--a purified turpentine,--is burnt, gives a flame

which emits most of the rays found in sunlight. Spirit of wine mixed

with water, warmed and ignited, gives only yellow rays; add nitrate

of strontian and they become red; but nitrate of barytes being mixed

with the fluid, they are changed to green and yellow; salts of copper

afford fine blue rays, and common salt intense yellow ones. Many of

these coloured rays and others can be produced in great power by the

use of various solid bodies introduced into flame. This has not been

sufficiently pointed out by authors; but it is clear from experiments

that light requires the presence of matter to enable it to diffuse its

coloured glories. How is it that the oxygen and hydrogen flame gives so

little light, and with a solid body present, pours forth such a flood

of brilliancy?

The production of artificial light by electrical and chemical agencies

will necessarily find some consideration under their respective

heads. There are numerous phenomena which connect themselves with

luminous power, or appear to do so, which, in the present state of

our knowledge, cannot come immediately under our attention. We are

compelled to reserve our limited space for those branches of science

which we are enabled to connect with the great natural operations

constantly going on around us. Many of these more abstruse results

will, however, receive some incidental notice when we come to examine

the operation of the combined physical forces on matter.

We see in light a principle which, if it has not its source in the

sun, is certainly dependent upon that luminary for its manifestations

and powers. From that “fountain of light” we find this principle

travelling to us at a speed which almost approaches the quickness of

thought itself; yet by the refinements of science we have been enabled

to measure its velocity with the utmost accuracy. The immortal poet of

our own land and language, in his creations of Ariel, that “tricksy

spirit,” who could creep like music upon the waters, and of the

fantastic Puck, who could girdle the earth in thirty minutes, appears

to have approached to the highest point to which mere imagination could

carry the human mind as to the powers of things ethereal. Science has,

since then, shown to man that this “spirit, fine spirit,” was a laggard

in his tasks, and a gross piece of matter, when compared with the

subtile essences which man, like a nobler Prospero, has now subdued to

do him service.

Light is necessary to life; the world was a dead chaos before its

creation, and mute disorder would again be the consequence of its

annihilation. Every charm which spreads itself over this rolling globe

is directly dependent upon luminous power. Colours, and probably,

forms, are the result of light; certainly the consequence of solar

radiations. We know much of the mysterious influences of this great

agent, but we know nothing of the principle itself. The solar beam has

been tortured through prismatic glasses and natural crystals; every

chemical agent has been tried upon it, every electrical force in the

most excited state brought to bear upon its operations, with a view

to the discovery of the most refined of earthly agencies; but it has

passed through every trial without revealing its secrets, and even the

effects which it produces in its path are unexplained problems, still

to tax the intellect of man.

Every animal and every plant alike proclaim that life and health are

due to light; and even the crystallizing forms of inorganic matter, by

bending towards it, confess its all-prevailing sway. From the sun to

each planet revolving around that orb, and to the remotest stars which

gleam through the vast immensity of heaven, we discover this power

still in its brightness, giving beauty and order to these unnumbered

creations; no less completely than to this small island of the universe

which we call our Earth. Through every form of matter we can mark

its power, and from all, we can, under certain conditions, evoke it

in lustre and activity. Over all and through all light spreads its

ethereal force, and manifests, in all its operations, powers which

might well exalt the mind of Plato to the idea of an omniscient and

omnipresent God. Science, with her Ithuriel wand, has, however, shown

that light is itself the effect of a yet more exalted cause, which we

cannot reach.

Indeed, the attentive study of the fine abstractions of science lifts

the mind from the grossness of matter, step by step, to the refinements

of immateriality, and there appear, shadowed out beyond the physical

forces which man can test and try, other powers still ascending, until

they reach the Source of every good and every perfect gift.

FOOTNOTES:

[84] “These--oxygen, hydrogen, nitrogen, and carbon--are the four

bodies, in fact, which, becoming animated at the fire of the sun,

the true torch of Prometheus, approve themselves upon the earth

the eternal agents of organisation, of sensation, of motion and of

thought.”--Dumas, _Leçons de Philosophie Chimique_, p. 100. Paris, 1837.

[85] It will be found in examining any of the works of the

alchemists,--particularly those of Geber, _De inveniendi arte Auri et

Argenti_, and his _De Alchemiâ_; Roger Bacon’s _Opus Majus, or Alchymia

Major_; Helvetius’ _Brief of the Golden Calf_; or Basil Valentine’s

_Currus Triumphalis_,--that in the processes of transmutation the solar

light was supposed to be marvellously effective. In Boyle’s _Sceptical

Chemist_ the same idea will be found pervading it.

Amid all their errors, the alchemists were assiduous workmen, and to

them we are indebted for numerous facts. Of them, and of their age, as

contrasted with our own, Gibbon remarks:--“Congenial to the avarice

of the human heart, it was studied in China, as in Europe, with equal

eagerness and equal success. The darkness of the middle ages ensured

a favourable reception to every tale of wonder; and the revival of

learning gave new vigour to hope, and suggested more specious arts

of deception. Philosophy, with the aid of experience, has at length

banished the study of alchemy; and the present age, however desirous of

riches, is content to seek them by the humbler means of commerce and

industry.”--_Decline and Fall_, vol. ii. p. 137.

[86] On the two theories the following maybe consulted:--Young,

_Supplement to Encyclopædia Britannica_, article _Chromatics_;

Fresnel, _Supplément à la Traduction Française de la 5ième édition du

Traité de Chimie de Thomson_, par Riffault, Paris, 1822; Herschel’s

Article, _Light_, in the Encyclopædia Metropolitana, and the French

Translation of it by Quetelet and Verhulst; Airy’s _Tract on the

Undulatory Theory_, in his Tracts, 2nd edition, Cambridge, 1831; Powel,

_The Undulatory Theory applied to Dispersion_, &c. p. 184; Lloyd’s

_Lectures_, Dublin, 1836-41; Cauchy, _Sur le Mouvement des Corps

élastiques_, Mémoires de l’Institut, 1827, vol. ix. p. 114; _Théorie de

la Lumière_, Ibid. vol. x. p. 293; M’Cullagh, _On Double Refraction_,

Ibid., vol. xvi.; _Geometrical Propositions applied to the Wave Theory

of Light_, Ibid., vol. xvii.; Sir David Brewster’s papers in the

Transactions of the Royal Society of Edinburgh, and the Philosophical

Magazine.

[87] _Results of Astronomical Observations made during the years

1834-38, at the Cape of Good Hope, &c._ By Sir John Herschel, Bart.,

K.H., D.C.L., F.R.S.--“In the contemplation of the infinite, in number

and in magnitude, the mind ever fails us. We stand appalled before this

mighty spectre of boundless space, and faltering reason sinks under the

load of its bursting conceptions. But, placed as we are on the great

locomotive of our system, destined surely to complete at least one

round of its ethereal course, and learning that we can make no apparent

advance on our sidereal journey, we pant with new ardour for that

distant bourne which we constantly approach without the possibility

of reaching it. In feeling this disappointment, and patiently bearing

it, let us endeavour to realise the great truth from which it flows.

It cannot occupy our mind without exalting and improving it.”--_Sir D.

Brewster_: North British Review.

[88] For examples of this, consult Graham’s _Elements of Chemistry_;

Brande’s _Manual of Chemistry_; or, indeed, any work treating of the

science. The formation of ink, by mixing two colourless solutions,

one of gallic acid and another of sulphate of iron, may be taken as a

familiar instance.

[89] Sir John Herschel, in his paper _On the Chemical Action of the

Rays of the Solar Spectrum on Preparations of Silver_, remarks that,

“it may seem too hazardous to look for the cause of this very singular

phenomenon in a real difference between the chemical agencies of those

rays which issue from the central portion of the sun’s disc, and those

which, emanating from its borders, have undergone the absorptive

action of a much greater depth of its atmosphere; and yet I confess

myself somewhat at a loss what other cause to assign for it. It must

suffice, however, to have thrown out the hint; remarking only, that

I have other, and, I am disposed to think, decisive evidence (which

will find its place elsewhere) of the existence of an absorptive solar

atmosphere, extending beyond the luminous one. The breadth of the

border, I should observe, is small, not exceeding 0·5 or 1/7 part of

the sun’s radius, and this, from the circumstances of the experiment,

must necessarily err in excess.”--Philosophical Transactions, 1840.

[90] _Experiments and Observations on some Cases of Lines in the

Prismatic Spectrum, produced by the passage of Light through Coloured

Vapours and Gases, and from certain Coloured Flames._ By W. A.

Miller, M.D., F.R.S., Professor of Chemistry in King’s College,

London.--Philosophical Magazine, vol. xxvii.

[91] _Report on the Mollusca and Radiata of the Ægean Sea, and on their

distribution, considered as bearing on Geology._ By Edward Forbes,

F.R.S., &c.--Reports of the British Association, vol. xii. Professor

Forbes remarks:--“A comparison of the testacea, and other animals of

the lowest zones, with those of the higher, exhibits a very great

distinction in the hues of the species, those of the depths being, for

the most part, white or colourless, while those of the higher regions,

in a great number of instances, exhibit brilliant combinations of

colour. The results of an enquiry into this subject are as follows:--

“The majority of shells of the lowest zone are white or transparent; if

tinted rose is the hue, a very few exhibit markings of another colour.

In the seventh region, white species are also very abundant, though

by no means forming a proportion so great as the eighth. Brownish

red, the prevalent hue of the brachiopoda, also gives a character

of colour to the fauna of this zone; the crustacea found in it are

red. In the sixth zone the colours become brighter, reds and yellows

prevailing,--generally, however, uniformly colouring the shell. In

the fifth region many species are banded or clouded with various

combinations of colours, and the number of white species has greatly

diminished. In the fourth, purple hues are frequent, and contrasts of

colour common. In the second and third, green and blue tints are met

with, sometimes very vivid; but the gayest combinations of colour are

seen in the littoral zone, as well as the most brilliant whites.

“The animals of Testacea, and the Radiata of the higher zones, are

much more brilliantly coloured than those of the lower, where they are

usually white, whatever the hue of the shell may be. Thus the genus

_Trochus_ is an example of a group of forms mostly presenting the

most brilliant hues both of shell and animal; but whilst the animals

of such species as inhabit the littoral zone are gaily chequered with

many vivid hues, those of the greater depth, though their shells are

almost as brightly covered as the coverings of their allies nearer the

surface, have their animals, for the most part, of a uniform yellow or

reddish hue, or else entirely white. The chief cause of this increase

of intensity of colour as we ascend is, doubtless, the increased amount

of light above a certain depth.”--p. 172.

[92] Ἁμὁρφωτα. _On the Epipolic Dispersion of Light_, being a paper

entitled, _On a case of Superficial Colour presented, by a homogeneous

liquid internally colourless_. By Sir J. F. W. Herschel, Bart, K.H.,

F.R.S., &c.--_An epipolized beam of light_ (meaning thereby a beam

which has once been transmitted through a quiniferous solution, and

undergone its dispersing action) _is incapable of further undergoing

epipolic dispersion_. In proof of this the following experiment may be

adduced,--

A glass jar being filled with a quiniferous solution, a piece of plate

glass was immersed in it vertically, so as to be entirely covered, and

to present one face directly to the incident light. In this situation,

when viewed by an eye almost perpendicularly over it, so as to graze

either surface very obliquely, neither the anterior nor posterior face

showed the slightest trace of epipolic colour. Now, the light, at its

egress from the immersed glass, entered the liquid under precisely the

same circumstances as that which, when traversing the anterior surface

of the glass jar, underwent epipolic dispersion on first entering

the liquid. It had, therefore, lost a property which it originally

possessed, and could not, therefore, be considered _qualitatively_ the

same light.--Philosophical Transactions, vol. cxxxvi.

[93] In connection with this view, the Newtonian theory should be

consulted, for which see--_A Letter of_ Mr. Isaac Newton, _Professor

of the Mathematicks in the University of Cambridge; containing his new

Theory about Light and Colors: sent by the Author to the Publisher,

from Cambridge, Feb. 6, 1671-72, in order to be communicated to the

Royal Society._

[94] In that admirable work, _The Physical Atlas_ of Dr. Berghaus, of

which a very complete edition by Alexander Keith Johnstone is published

in this country, the following order of the distribution of plants is

given:--

1. The region of palms and bananas Equatorial zone.

2. Tree ferns and figs Tropical zone.

3. Myrtles and laurels Sub-tropical zone.

4. Evergreen trees Warm temperate zone.

5. European trees Cold temperate zone.

6. Pines Sub-arctic zone.

7. Rhododendrons Arctic zone.

8. Alpine plants Polar zone.

Consult Humboldt, _Essai sur la Géographie des Plantes_, Paris,

1807; _De Distributione Geographicâ Plantarum_, Paris, 1817. Schouw,

_Grundzüge der Pflanzengeographie_. Also his _Earth, Plants, and Man_;

translated by Henfrey, in _Bohn’s Scientific Library_. Lamouroux,

_Géographie Physique_. _The Plant, a Biography_: by Schleiden;

translated by Henfrey. _Physical Geography_: by Mrs. Somerville.

[95] Fraunhofer’s measure of illuminating power is as follows:--

At the 22nd degree of the red 0·032

" 34th degree of the red 0·094

" 22nd degree of the orange 0·640

" 10th degree of the yellow 1·000

" 42nd degree of the yellow 0·480

" 2nd degree of the blue 0·170

" 16th degree of the indigo 0·031

" 43rd degree of the violet 0·0056

[96] Herschel, _On the Action of Crystallized Bodies on Homogeneous

Light, and on the causes of the deviation from Newtons scale in

the tints which many of them develope on exposure to a polarized

ray_.--Phil. Trans., vol. cx., p. 88.

[97] _On the Nature of Light and Colours_: Lecture 39, in Young’s

_Lectures on Natural Philosophy_, Kelland’s Edition, p. 373, and the

authorities there quoted.

[98] Brewster’s _Optics_: Lardner’s Cabinet Cyclopædia. Herschel, _On

Light_: Encyclopædia Metropolitana.

[99] Malus, _Sur une Propriété de la Lumière Réfléchie_: Mémoires

d’Arcueil. Numerous memoirs by Sir David Brewster, in the Philosophical

Transactions.

[100] Bartholin, _On Iceland Crystals_: Copenhagen, 1669. _An

Accompt of sundry Experiments made and communicated by that Learn’d

Mathematician_ Dr. Erasmus Bartholin, _upon a Chrystal like Body sent

to him out of Island_: in connection with which Dr. Matthias Paissenius

writes:--The observations of the excellent Bartholin upon the Island

Chrystal are, indeed, considerable, as well as painful. We have here,

also, made some tryals of it upon a piece he presented me with, which

confirm his observations. Mean time he found it somewhat scissile and

reducible by a knife into thin laminas or plates, which, when single,

shew’d the object single, but laid upon one another shew’d it double;

the two images appearing the more distant from one another, the

greater the number was of those thin plates laid on one another. With

submission to better judgements I think it to be a kind of Selenites.

Some of our curious men here were of opinion that the Rhomboid figure

proper to this stone was the cause of the appearances doubled thereby.

But having tryed whether in other transparent bodies of the like figure

the like would happen, we found no such thing in them, which made us

suspect some peculiarity in the very Body of the stone.--Phil. Trans.

for 1670, vol. v.

[101] _On the Application of the Laws of Circular Polarization to the

Researches of Chemistry_: by M. Biot.--Nouvelles Annales du Muséum

d’Histoire Naturelle, vol. iii., and Scientific Memoirs, vol. i.

p. 600. _On Circular Polarization_: by Dr. Leeson.--Memoirs of the

Chemical Society.

[102] In Sir David Brewster’s Treatise _On Optics_, chap, xviii., _On

Polarization_, the best arrangements for a polarizing apparatus will be

found described.

[103] This beautiful application was recently made by Professor

Wheatstone, the particulars of which will be found in his interesting

communication.--_On a means of determining the apparent Solar Time

by the diurnal changes of the Plane of Polarization at the Northern

Pole of the Sky_: Report of the Eighteenth Meeting of the British

Association.

[104] _On the Polarization of the Chemical Rays of Light_: by John

Sutherland, M.D., in which the author refers to the following

experiment of M. J. E. Bérard--“I received the chemical rays directed

into the plane of the meridian on an unsilvered glass, under an

incidence of 35° 61'. The rays reflected by the first glass were

received upon a second, under the same incidence. I found that when

this was turned towards the south, the muriate of silver exposed to

the invisible rays which it reflected was darkened in less than half

an hour; whereas, when it was turned towards the west, the muriate

of silver exposed in the place where the rays ought to have been

reflected, was not darkened, although it was left exposed for two

hours. It is consequently to be presumed that the chemical rays can

undergo double refraction in traversing certain diaphanous bodies; and

lastly, we may say that they enjoy the same physical properties as

light in general.”--Philosophical Magazine, vol. xx.

Dr. Leeson has stated that Daguerreotype pictures can be taken more

readily under the influence of polarized light, than by ordinary

radiation.

[105] _On the Magnetization of Light, and the Illumination of Magnetic

Lines of Force_: by Michael Faraday, D.C.L., F.R.S.--Philosophical

Transactions, vol. cxxxvii.--The following remarks are to the point

of doubt referred to in the text.--“The magnetic forces do not act

on the ray of light directly and without the intervention of matter,

but through the mediation of the substance in which they and the ray

have a simultaneous existence; the substances and the forces giving to

and receiving from each other the power of acting on the light. This

is shown by the non-action of a vacuum, of air or gases, and it is

also further shown by the special degree in which different matters

possess the property. That magnetic force acts upon the ray of light

always with the same character of manner, and in the same direction,

independent of the different varieties of substance, or their states

of solid or liquid, or their specific rotative force, shows that

the magnetic force and the light have a direct relation; but that

substances are necessary, and that these act in different degrees,

shows that the magnetism and the light act on each other through the

intervention of the matter. Recognising or perceiving _matter_ only by

its powers, and knowing nothing of any imaginary nucleus abstract from

the idea of these powers, the phenomena described must strengthen my

inclination to trust in the views I have advanced in reference to its

nature.”--Phil. Mag. vol. xxiv.

[106] The invention of the camera obscura certainly belongs to

Giambattista Porta, and is described in his _Magiæ Naturalis, sive de

Miraculis Rerum Naturalium, Libri Viginti_; Antwerp, 1561. An English

translation made in 1658 exists, but I have not seen it.

Hooke, in one of the earliest volumes of the Philosophical

Transactions, describes as new many of the phenomena mentioned by

Porta, and particularly the images of the dark chamber.

[107] Herschel, _On Light_,--Encyclopædia Metropolitana.

[108] “I would here observe that a consideration of many such

phenomena (the obliteration and revival of photographic drawings) has

led me to regard it as not impossible that the retina itself may be

_photographically_ impressed by strong light, and that some at least

of the phenomena of visual spectra and secondary colours may arise

from the sensorial perception of actual changes in progress in the

physical state of that organ itself subsequent to the cessation of the

direct stimulant.”--_On the action of the Rays of the Solar Spectrum on

Vegetable Colours, &c._: by Sir J. F. W. Herschel, Bart.

[109] Dumeril.

[110] _Theory of Colours_: by Goethe; translated by Eastlake.

[111] See Tuckey’s Narrative of the Expedition of the Zaire.

[112] The most complete examination of this subject will be found in

two Memoirs:--

1. _Experiments and observations on the light which is spontaneously

emitted with some degree, of permanency from various bodies._--Phil.

Trans., vol. xc.

2. _A continuation of the above, with some experiments and observations

on solar light, when imbibed by Canton’s phosphorus_: by Nathaniel

Hulm, M.D.--Phil. Trans., vol. xci.; and in the _Monograph of the

British Naked-eyed Medusæ_, by Professor Edward Forbes (published

for the Ray Society). See Wilson’s note to the account of _Pennalata

phosphorea_ in Johnston’s Zoophytes, 2nd edition.

[113] _A General Outline of the Animal Kingdom_: by Thomas Rymer Jones,

F.L.S.--Acalephæ, p. 64. _Lettre à M. Dumas sur la Phosphorescence des

Vers luisants_: par M. Ch. Matteucci.--Annales de Chimie, vol. ix. p.

71, 1843.

[114] _Memoirs of Benvenuto Cellini--Bohn’s Standard Library._ See also

his Treatise on his Art as a Sculptor and Engraver. Florence, 1568. 4to.

[115] _Phosphorescence of the Diamond_: by M. Reiss (Revue Scientifique

et Industrielle, vol. xxiii. p. 185).--“The diamond, phosphorescent

by insulation, lost rapidly its phosphorescence when submitted to the

action of the red rays of the solar spectrum. On the contrary, the

blue rays are those which render the diamond the most luminous in

the dark. It is probable that the phosphorescence produced by heat

is equally diminished by the action of the red rays of the solar

spectrum.” Giovanni Battista Beccaria published his experiments in

1769. See Priestley’s _History of Electricity_; and _On the Effects

of Electricity upon Minerals which are Phosphorescent by Heat_; and

_Further Experiments on the communication of Phosphorescence and Colour

to bodies of Electricity_; by Thomas J. Pearsall.--Journal of the

Royal Institution of Great Britain, Oct. 1830, Feb. 1831.--These two

memoirs contain the most complete set of experiments on this subject

which have yet been made; see _Placidus Heinrich_, _Phosphorescenz

der Körper_, vol. iv.; Gmelin’s _Handbuch der Chemie_, part 1.;--_On

the Phosphorescence of Minerals_, Brewster: Edinburgh Philosophical

Journal, vol. i. p. 137.;--_The Aërial Noctiluca, or some New

Phenomena, and a process of a factitious self shining substance_:

Boyle’s Works, vol. iv.

[116] _Des Effets produits sur les corps par les Rayons Solaires_: par

M. Edmond Becquerel.--Annales de Chimie, vol. ix. p. 257. 1843.

M. Becquerel has applied the term _phosphorogénique_ to those rays

producing phosphorescence.

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