CHAPTER II.

PROPERTIES OF MATTER.

17. =Variety in the Properties of Matter.=--All matter has

properties or qualities. Some of these are different in the

different kinds of matter. Thus its three forms have different

properties, as you saw in Chapter I. There is variety also in the

properties of substances of the same class. Thus liquids are unlike

each other in some respects. Some, for example, are lighter than

others. Oil is lighter than water. Gaseous substances also differ

in this and in other respects. But the variety in the properties

of solids is greater than in those of gases or liquids. This will

appear as I proceed.

18. =Divisibility of Matter.=--Any visible portion of matter can

be divided into parts. Even if it be so small that you can see

it only with a powerful microscope, it could still be divided if

you could have an instrument sufficiently fine for the purpose.

_Divisibility_, then, is said to be a _general_ property of matter;

that is, a property belonging to all kinds of matter.

19. =Examples of Minute Division of Matter.=--There are numerous

examples in which the division of matter is carried far beyond that

which can be effected by any cutting instrument. Some of these I

will notice:

A gold-beater can hammer a grain of gold into a leaf covering a

space of fifty square inches. So thin is it that it would take

282,000 of such leaves, laid upon each other, to make the thickness

of an inch. And yet so even and perfect is this thin layer of

gold, that when it is laid upon any surface in gilding it has the

appearance of solid gold. A fifty millionth part of this grain of

gold thus hammered out can be seen by the aid of a microscope which

magnifies the diameter of an object ten times. But the division of

gold is made even more minute than this in the manufacture of the

wire of gold-lace. It is done in this way: A bar of silver weighing

180 ounces is covered with a layer of gold weighing an ounce. It is

then drawn through a series of holes in a steel plate, diminishing

in diameter, till it at length comes out a very fine wire 4000 feet

long. Each foot of it then has only the one 4000th part of the

ounce of gold, and yet the silver is well covered.

A soap-bubble is a beautiful example of the minute division of

matter. That thin wall which incloses the air which you have blown

into it is composed of particles of the soap and of the water

mingled together. It is supposed to be less than one millionth of

an inch in thickness.

The thread of the silk-worm is so minute that the finest

sewing-silk is formed of many of these threads twisted together.

But the spider spins much more finely than this. The thread by

which you see him letting himself down from any height is made up

of about 6000 threads or filaments, each coming from a separate

hole in his spinning machine. A quarter of an ounce of the thread

of a spider's web would extend 400 miles.

A grain of blue vitriol, dissolved in a gallon of water, will

make the whole blue. Such a diffusion could not be without an

exceedingly minute division of the particles.

Perhaps the most minute division of matter is exemplified in odors.

A grain of musk will scent a room for years, and yet have no

perceptible loss of weight. But all this time the air is filled

with fine particles coming from the musk.

The microscope reveals to us many wonderful examples of the

minuteness of the particles of matter, both in the vegetable and

the animal world.

If you press a common puff-ball a dust flies off like smoke.

Examined with a microscope, each particle of this dust, which is

the seed of the plant, is a perfectly round orange-colored ball.

This ball is of course made up of very many particles, arranged in

this regular form. Beautiful examples of various arrangements of

the minute particles of matter we have in the pollen of different

plants, as seen with the microscope.

Each particle of the dust which adheres to your fingers as you

catch a moth is a scale with fine lines upon it regularly arranged.

And if you look through the microscope at the wing of the moth, you

will see, where the dust is rubbed off, the attachments by which

the scales were held standing up from the surface of the wing, like

nail-heads on a roof where the shingles have been torn off.

The organization of exceedingly small animals, as revealed by the

microscope, furnishes us with wonderful examples of the minute

division of matter. A little of the dust of guano, examined through

a powerful microscope, is seen to contain multitudes of shells

of various shapes. These shells are the remains of animalcules

that lived in the water, their destiny seeming to be in part to

furnish food to other animals larger than themselves. In the chalk

formations of the earth are seen multitudes of such shells. They

have been discovered even in the glazing of a visiting-card; for

they are so small that the fine grinding up of the chalk does not

wholly destroy them. There are animals, both in the air and in the

water, so small that it would take millions of them to equal in

bulk a gram of sand, and a thousand of them could swim side by side

through the eye of a common-sized needle. Now in all these animals

there are organs, constructed of particles of matter, which are

arranged in them with as much order and symmetry as in the organs

of our bodies. How minute then must these particles be!

How do such facts extend our views of the power of the Deity! The

same power that moulded the earth, sun, moon, and the whole "host

of heaven," gave form, and life, and motion to the millions which

sport in every sunbeam; the same eye that watches the immense

heavenly bodies as they move on in their course, looks upon one and

all of these legions of animals in earth, air, and water, though

they are unseen by human eyes, seeing that every particle shall

take its right position, so that this part of creation may with all

the rest be pronounced very good; and the same bountiful hand that

dispenses the means of life and enjoyment to the millions of the

human race, forgets not to minister to the brief life and enjoyment

of each one of these myriads of animalcules, though they seem to be

almost nothingness itself.

20. =Pores and Spaces in Matter.=--In all matter there are spaces

about the particles. Those bodies which are called porous have

quite large spaces in them. But even in those which are not

commonly considered porous the particles are by no means close

together. A celebrated experiment tried in Florence a long time

ago showed that there are spaces among the particles of so dense

a substance as gold sufficiently large to let water through them.

A hollow golden globe containing water was subjected to great

pressure, and its surface was bedewed with the water that came out

through the pores of the gold. In all substances in which there are

pores visible to the naked eye, or by the aid of the microscope,

there are other spaces or interstices among the particles around

the pores. Indeed, it is supposed that there is space around every

ultimate particle or atom, and that no two of these atoms are

in actual contact. The fact that substances which have no pores

can be compressed into a smaller space than they usually occupy

shows that there are spaces or interstices in them. Solids can be

thus compressed, some more than others. But the most compressible

substances are the gases and vapors. The amount of space between

their particles must be very large to allow of so great compression.

[Illustration: Fig. 1.]

21. =Space in Gaseous Substances.=--We can have some idea of

the great amount of space in a gaseous or aeriform substance by

observing the difference between water in its liquid and in its

aeriform state. A cubic inch of water, when it becomes steam,

occupies 1696 times as much room as it did when it was water. The

difference in proportion is exhibited in Fig. 1, the inner circle

representing the water, and the outer the steam into which it is

converted. Now the water is not altered at all in its nature by

being changed into steam. The particles are simply put farther

apart by the heat, and as soon as the heat is withdrawn they

come together again to form water, or, in other words, the steam

is condensed into water. It is plain, therefore, that the space

between the particles is 1696 times as great in steam as it is in

the water from which the steam is made.

22. =Solutions.=--When any substance, as sugar or salt, is

dissolved in water, its particles are diffused through the spaces

that exist between the particles of the water. So also when water

evaporates (§ 12), the particles of water are diffused through the

spaces between the particles of the air. In like manner are the

particles from an odorous substance diffused in these spaces, and

thus mingled with the particles of the air they are carried into

the nostrils, and strike upon the minute extremities of the nerve

of smell.

23. =Relation of Heat to the Spaces of Matter.=--The variation

in the amount of space between the particles of matter in any

substance generally depends on the variation of the amount of

heat present. Thus heat expands iron; that is, it increases the

spaces between the particles of the iron. So also heat increases

the spaces between the particles of mercury, and thus makes it

occupy more room in the thermometer. This effect of heat will be

considered more fully hereafter.

The general views which I have given of the constitution of

matter will throw light upon the different qualities of different

substances, some of which I will notice.

24. =Density and Rarity.=--The density of a substance depends upon

the quantity of matter it contains in a given space. The more

dense, therefore, a substance is the greater is its weight. A piece

of lead is forty times heavier than a piece of cork of the same

size. Mercury is nearly fourteen times heavier than an equal bulk

of water. You see, then, that density must depend on the nearness

of the atoms to each other. In so dense a substance as gold the

atoms are all very close together; in wood there are spaces, some

of which are so large that you can see them; and in air, steam, and

the gases there is a great deal of space among the particles (§

21), so that we speak of their _rarity_ instead of their density.

25. =Tenacity.=--The power of holding together, termed tenacity,

depends on the degree of attraction between the particles. By

attraction I mean a disposition in particles to come together, this

disposition being manifested in opposition to any force tending

to draw them apart. I shall soon speak of this more particularly.

Tenacity does not exist at all in gaseous substances. The particles

of air and of steam, for example, show no disposition to cling

together; that is, have no tenacity. This property is weak in

liquids. It is only strong enough in water to enable its particles

to hang together in the shape of a drop. It is strong in solids,

enabling their particles not only to hold together in large

quantities, but to hold up also heavy weights suspended to them.

It is stronger in iron than in any other solid. It is stronger in

wrought iron than in cast iron; and strongest of all in steel.

26. =Comparative Tenacity of Substances.=--Various metals and other

substances have been tested in reference to their comparative

tenacity. It was done in this way: Wires were made of the metals,

all of the same size. Weights were suspended to them, and additions

were made to the weights by little and little till the wires broke.

The table underneath was made by placing against each metal the

greatest weight that its wire would hold:

Cast steel 134 pounds.

Best wrought iron 70 pounds.

Cast iron 19 pounds.

Copper 19 pounds.

Silver 11 pounds.

Gold 9 pounds.

Tin 5 pounds.

Lead 2 pounds.

Oak wood, tried in the same way, was found to hold up 12 pounds,

one more pound than silver. Some animal substances have great

tenacity, as the thread of the silk-worm, hair, wool, and the

ligaments and tendons of our bodies and of other animals.

27. =Value of Tenacious Substances.=--"The gradual discovery," says

Dr. Arnot, "of substances possessed of strong tenacity, and which

man could yet easily mould and apply to his purposes, has been of

great importance to his progress in the arts of life. The place of

the hempen cordage of European navies is still held in China by

twisted canes and strips of bamboo; and even the hempen cable of

Europe, so great an improvement on former usage, is now rapidly

giving way to the more complete and commodious security of the iron

chain--of which the material to our remote ancestors existed only

as useless stone or earth. And what a magnificent spectacle is it,

at the present day, to behold chains of tenacious iron stretched

high across a channel of the ocean, as at the Menai Strait between

Anglesea and England, and supporting an admirable bridge-road of

safety, along which crowded processions may pour, regardless of

the deep below, or of the storm; while ships there, with sails

full-spread, pursue their course unmolesting and unmolested."

28. =Hardness.=--This property seems to depend upon some peculiar

arrangement of the particles of matter. We should suppose that the

densest substances would be the hardest. But it is not so. Iron

is the hardest of the metals, but its particles are not so close

together as those of gold, which is quite a soft metal. And gold

is five times as heavy as the diamond, which is so hard as to cut

glass easily. Common flint is hard enough to scratch glass, but

will not cut it like the diamond.

[Illustration: Fig. 2.]

29. =Flexibility and Brittleness.=--If you bend a flexible body as

a piece of wood, as represented in Fig. 2, it is obvious that the

particles on the upper or convex side must be put a little farther

apart, while those on the under or concave side are brought a

little nearer together. But the wood does not break, because the

particles that are thus moved a little apart still retain their

hold upon each other. This is the explanation of what we call

flexibility. On the other hand, the particles in a rod of glass

can not be put farther apart in this way. They are not actually in

contact any more than the particles of the wood are (§ 20), but

they are in a _fixed_ relative position; that is, a position which

can not be disturbed without a _permanent_ separation of particles.

If you attempt to bend the rod there is no slight separation of

many particles, as in the bent wood, but a full and permanent

separation in some one part of the rod. We call the property on

which this result depends brittleness. Brittle substances are

generally hard. Glass, while the most brittle of all substances,

is hard enough to scratch iron. Brittle substances also have much

tenacity. A rod of glass can hold up a heavy weight, although a

slight blow suddenly given would break it.

30. =Flexible and Brittle Steel.=--There are two kinds of steel,

flexible and brittle. The steel of most cutting instruments is

brittle. The steel of a sword-blade is quite flexible, and that

of a watch-spring is so much so that we can wind it up in a coil.

This difference is owing to a difference in the mode of cooling

the steel. If it be cooled suddenly, it is brittle; if slowly,

it is flexible. The process by which it is cooled slowly is

called _annealing_. The explanation of all this is quite plain.

The steel being expanded by heat--that is, its particles being

put farther apart than they usually are--when they are suddenly

brought together again they have not time to arrange their relative

position properly. Brittleness is therefore the result. But, on the

other hand, when the cooling is effected gradually, time is given

for the arrangement.

31. =Tempering of Steel.=--Steel suddenly hardened is too brittle

for common use. A process called tempering is therefore resorted

to for diminishing the brittleness. The steel is reheated after

the hardening, and is then allowed to cool slowly. The degree in

which the brittleness is lessened depends on the degree of heat to

which the steel is subjected. It can be entirely removed by a red

heat, for then the particles have a full opportunity to readjust

themselves; and the more the heat comes short of this point the

less thorough will be the adjustment, because the less perfectly

are the particles released from their suddenly-taken position. In

lessening the brittleness we lessen hardness also, and therefore

the tempering is varied in different cases according to the degree

of hardness which is desired.

32. =Annealing of Glass.=--Glass is always annealed. If this

were not done our glass vessels and windows would be exceedingly

brittle, and would therefore be constantly breaking. Articles made

of glass are annealed by being passed very slowly indeed through

a long oven which is very hot at one end, the heat gradually

lessening toward the other end.

[Illustration: Fig. 3]

33. =Prince Rupert's Drops.=--We have a striking example of

brittleness induced by sudden cooling in what are called Prince

Rupert's drops. These are made by dropping melted green glass into

cold water, and they are of the shape represented in Fig. 3. If

you break off ever so small a bit of the point of one of these

drops, the whole will at once shiver to pieces. That is, the sudden

arrangement of the particles is so slight and unnatural that the

disturbance of the arrangement in a small part suffices to destroy

the arrangement of the whole, very much as a row of bricks falls

over from the fall of the first in the row. Mr. Farraday says that

these drops were not, as is commonly supposed, invented by Prince

Rupert, but were first brought to England by him in 1660. They

excited much curiosity at that time, and were considered "a kind of

miracle in nature." But you see that this, like many other wonders,

receives with a little thought an easy explanation.

34. =Malleability and Ductility.=--Those metals which can be

hammered into thin plates are called malleable. Gold furnishes us

with the best illustration of this property. Silver, copper, and

tin are quite malleable. Most of the other metals are very little

so, and some of them are not at all, breaking at the first blow.

A substance is said to be _ductile_ when it can be drawn out into

wire. The principal metals that have this quality are platinum,

silver, iron, copper, and gold, and in the order in which I have

named them. Melted glass is very ductile. It can be drawn out in

a very fine thread, and when this thread is cut and arranged in

branches it resembles beautiful white hair. In hammering metals

into plates, or drawing them into wire, there is a considerable

change of relative position in the particles, similar to that which

we have in fluids, though nothing like as free. In this change of

position those particles that do remain in close neighborhood have

a remarkable tenacity or attraction, preventing their separation.

In welding two pieces of iron, which is done by the blacksmith by

hammering them together when red-hot, there must be enough movement

among the particles to have those of one piece mingle somewhat with

those of the other.

35. =Compressibility.=--Porous substances can be considerably

compressed. Force applied to them can bring their particles

nearer together, making them to fill up in part their pores. The

most familiar example you have of this is in sponge. The more

porous wood is the more can it be compressed. But even such dense

substances as the metals can be compressed in some degree; that is,

the interstices between their particles can be made smaller. Medals

and coins have their figures and letters stamped upon them by

pressure, just as impressions are made upon melted sealing-wax. The

heavy and quick pressure required to do this actually compresses

the whole piece of the hard metal, putting all the particles nearer

together, so that it occupies less space than it did before it was

stamped.

36. =Incompressibility of Liquids.=--We should suppose, from the

freeness with which the particles of liquids move among each

other, and from the spaces (§ 22) which exist among them, that

these substances could be easily compressed. But it is not so. The

heaviest pressure is required to compress them even in a slight

degree. Water can be compressed so very little that practically it

is regarded as incompressible.

37. =Influence of Heat on the Bulk of Liquids.=--Although the

interstices between the particles of liquids can not be varied by

mechanical pressure, they can be by variations of temperature.

Liquids are dilated or expanded by heat; that is, their particles

are put farther apart. They are contracted or compressed by cold;

that is, their particles are brought nearer together by the

abstraction of heat. The most familiar example that we have is

in the thermometer. The mercury rises in the tube when the heat

increases the interstices between its particles; and it falls when

the loss of heat allows the particles to come near together. The

same effects are seen when alcohol is used in the thermometer,

as is done in the arctic regions, because mercury may freeze

there. A thermometer with water in it would answer if we wished

only to measure temperatures between the freezing point and the

boiling point of water. The expansive influence of heat will be

particularly treated of hereafter.

38. =Compressibility of Aeriform Substances.=--Aeriform bodies

are more compressible than any other substances, showing that in

their ordinary condition there is a great deal of space among their

particles. While they are thus unlike liquids in compressibility,

they are affected by heat in the same way that liquids are.

[Illustration: Fig. 4. Fig. 5.]

39. =Elasticity.=--Closely allied with the compressibility

of matter is its elasticity. We see this property strikingly

exemplified in India-rubber. It occasions the rebounding of a ball

of this substance when thrown down. Observe flow exactly what

occurs in this case. The ball as it meets the resistance of the

floor is flattened, as represented in Fig. 4. Then, as it assumes

the round shape, as seen in Fig. 5, it pushes downward upon the

floor. It is this sudden pushing downward that makes it rebound.

It is as if there were a compressed spring between the ball and

floor. It may be likened also to jumping. When one jumps he bends

his limbs at the thigh and knee joints, and then, in straightening

himself up, gives a sudden push, like that given by the ball as

it assumes its round shape, and so is thrown forward or upward,

according to the direction in which the pushing force is made.

The same flattening occurs in an ivory ball, though not to the

same degree. You can prove that it does occur by experiment. Let a

marble slab be wet and drop the ball upon it. Quite a spot will be

made dry by the blow of the ball, showing that it touched more of

the marble than it does when it is merely placed upon it.

40. =Elasticity Shown in Other Ways.=--If a stick be bent, as in

Fig. 2, as soon as the bending force is withdrawn the stick becomes

straight again from its elasticity. It is this elastic force of the

bow, straightening it, that speeds the arrow. Observe in this case

that while the particles on the concave side of the bent bow are

brought nearer together or compressed, those on the convex side are

moved apart. This moving apart of the particles is often shown in

India-rubber. You can see how very far apart particles that are in

near neighborhood may be carried, if you will stick two pins close

together in a strip of India-rubber before you stretch it.

41. =Degrees of Elasticity in Different Substances.=--Some

substances have so very little elasticity that they are practically

considered as having none. Lead is one of these. A rod of lead

when bent remains so, and a leaden ball does not rebound. While

aeriform substances are the most compressible of all, they are also

the most elastic. Air compressed returns to its usual condition

the moment that it is relieved from the pressure, and with a force

proportioned to the amount of the pressure. So it is with steam

and the gases. The varied results of this quality of aeriform

substances will claim our attention more particularly in some

other parts of this book.

42. =Definition of Elasticity.=--You see from the illustrations

that have been given that elasticity is _that property of matter

by which its particles, when brought nearer together or carried

farther apart by any force, return to their usual condition when

the force is withdrawn_.

43. =Usefulness of Variety in Properties of Matter.=--The

various properties of matter brought to view in this chapter are

providential adaptations to the necessities of man. Each substance

has those properties which best fit it for his use. Iron, for

example, designed by the Creator to be both the strongest and most

extensively useful servant of man among the metals, is therefore

provided in great abundance, and has those strong, decided, and

various qualities which fit it for the services it is to perform.

Gold and silver, on the other hand, designed for services less

extensive, lighter, and in a great measure ornamental, are provided

in very much less quantity, and have properties admirably adapting

them to the services for which they are so manifestly intended.

The same can be substantially said of all other substances, and

especially of those very abundant ones, air and water. And it

may be remarked also that the ingenuity of man is continually

discovering new modes of bringing the various properties of matter

into his service. I will give but a single illustration--the

tempering of steel. "This discovery," says Dr. Arnot, "is perhaps

second in importance to few discoveries which man has made; for it

has given him all the edge-tools and cutting-instruments by which

he now moulds every other substance to his wishes. A savage will

work for twelve months with fire and sharp stones to fell a great

tree and to give it the shape of a canoe, where a modern carpenter,

with his tools, could accomplish the object in a day or two."

Science for the School and Family, Part I. Natural Philosophy · 第 2 / 16 章