CHAPTER VI.

METHODS OF OBSERVATION.--MINOR METHODS.

I.--CONCOMITANT VARIATIONS.

_Whatever phenomenon varies in any manner whenever another

phenomenon varies in some particular manner, is either a

cause or an effect of that phenomenon, or is connected with it

through some fact of causation._

This simple principle is constantly applied by us in connecting and

disconnecting phenomena. If we hear a sound which waxes and wanes with

the rise and fall of the wind, we at once connect the two phenomena.

We may not know what the causal connexion is, but if they uniformly

vary together, there is at once a presumption that the one is causally

dependent on the other, or that both are effects of the same cause.

This principle was employed by Wells in his researches into Dew. Some

bodies are worse conductors of heat than others, and rough surfaces

radiate heat more rapidly than smooth. Wells made observations on

conductors and radiators of various degrees, and found that the

amount of dew deposited was greater or less according as the objects

conducted heat slowly or radiated heat rapidly. He thus established

what Herschel called a "scale of intensity" between the conducting and

radiating properties of the bodies bedewed, and the amount of the dew

deposit. The explanation was that in bad conductors the surface cools

more quickly than in good conductors because heat is more slowly

supplied from within. Similarly in rough surfaces there is a more

rapid cooling because heat is given off more quickly. But whatever

the explanation might be, the mere concomitant variation of the

dew deposit with these properties showed that there was some causal

connexion between them.

It must be remembered that the mere fact of concomitant variation is

only an index that some causal connexion exists. The nature of

the connexion must be ascertained by other means, and may remain

a problem, one of the uses of such observed facts being indeed to

suggest problems, for inquiry. Thus a remarkable concomitance has been

observed between spots on the sun, displays of Aurora Borealis, and

magnetic storms. The probability is that they are causally connected,

but science has not yet discovered how. Similarly in the various

sciences properties are arranged in scales of intensity, and any

correspondence between two scales becomes a subject for investigation

on the assumption that it points to a causal connexion. We shall see

afterwards how in social investigations concomitant variations in

averages furnish material for reasoning.

When two variants can be precisely measured, the ratio of the

variation may be ascertained by the Method of Single Difference. We

may change an antecedent in degree, and watch the corresponding change

in the effect, taking care that no other agent influences the effect

in the meantime. Often when we cannot remove an agent altogether,

we may remove it in a measurable amount, and observe the result. We

cannot remove friction altogether, but the more it is diminished, the

further will a body travel under the impulse of the same force.

Until a concomitant variation has been fully explained, it is merely

an empirical law, and any inference that it extends at the same

rate beyond the limits of observation must be made with due caution.

"Parallel variation," says Professor Bain, "is sometimes interrupted

by critical points, as in the expansion of bodies by heat, which

suffers a reverse near the point of cooling. Again, the energy of a

solution does not always follow the strength; very dilute solutions

occasionally exercise a specific power not possessed in any degree

by stronger. So, in the animal body, food and stimulants operate

proportionally up to a certain point, at which their further operation

is checked by the peculiarities in the structure of the living

organs.... We cannot always reason from a few steps in a series to the

whole series, partly because of the occurrence of critical points,

and partly from the development at the extremes of new and unsuspected

powers. Sir John Herschel remarks that until very recently 'the

formulae empirically deduced for the elasticity of steam, those for

the resistance of fluids, and on other similar subjects, have almost

invariably failed to support the theoretical structures that have been

erected upon them'."[1]

II.--SINGLE RESIDUE.

_Subduct from any phenomenon such part as previous induction

has shown to be the effect of certain antecedents, and the

residue of the phenomenon is the effect of the remaining

antecedents._

"Complicated phenomena, in which several causes concurring, opposing,

or quite independent of each other, operate at once, so as to produce

a compound effect, may be simplified by subducting the effect of all

the known causes, as well as the nature of the case permits, either by

deductive reasoning or by appeal to experience, and thus leaving as it

were a _residual phenomenon_ to be explained. It is by this process,

in fact, that science, in its present advanced state, is chiefly

promoted. Most of the phenomena which nature presents are very

complicated; and when the effects of all known causes are estimated

with exactness, and subducted, the residual facts are constantly

appearing in the form of phenomena altogether new, and leading to the

most important conclusions."[2]

It is obvious that this is not a primary method of observation, but

a method that may be employed with great effect to guide observation

when a considerable advance has been made in accurate knowledge

of agents and their mode of operation. The greatest triumph of the

method, the discovery of the planet Neptune, was won some years after

the above passage from Herschel's Discourse was written. Certain

perturbations were observed in the movements of the planet Uranus:

that is to say, its orbit was found not to correspond exactly with

what it should be when calculated according to the known influences

of the bodies then known to astronomers. These perturbations were a

residual phenomenon. It was supposed that they might be due to

the action of an unknown planet, and two astronomers, Adams and Le

Verrier, simultaneously calculated the position of a body such as

would account for the observed deviations. When telescopes were

directed to the spot thus indicated, the planet Neptune was

discovered. This was in September, 1846: before its actual discovery,

Sir John Herschel exulted in the prospect of it in language that

strikingly expresses the power of the method. "We see it," he said,

"as Columbus saw America from the shores of Spain. Its movements have

been felt, trembling along the far-reaching line of our analysis, with

a certainty hardly inferior to that of ocular demonstration."[3]

Many of the new elements in Chemistry have been discovered in this

way. For example, when distinctive spectrums had been observed for all

known substances, then on the assumption that every substance has a

distinctive spectrum, the appearance of lines not referable to any

known substance indicated the existence of hitherto undiscovered

substances and directed search for them. Thus Bunsen in 1860

discovered two new alkaline metals, Caesium and Rubidium. He was

examining alkalies left from the evaporation of a large quantity of

mineral water from Durkheim. On applying the spectroscope to the flame

which this particular salt or mixture of salts gave off, he found that

some bright lines were visible which he had never observed before, and

which he knew were not produced either by potash or soda. He then set

to work to analyse the mixture, and ultimately succeeded in separating

two new alkaline substances. When he had succeeded in getting them

separate, it was of course by the Method of Difference that he

ascertained them to be capable of producing the lines that had excited

his curiosity.

[Footnote 1: Bain's _Logic_, vol. ii. p. 64.]

[Footnote 2: Herschel's _Discourse_, Sec. 158.]

[Footnote 3: De Morgan's _Budget of Paradoxes_, p. 237.]

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