Page images
PDF
EPUB
[blocks in formation]

minum and iron, copper and iron and other combinations may be used, except that there is a loss in sensitiveness in the order indicated. Two pieces or strips E and E', each about 9.0 mm. in width and 6.0 mm. thickness are riveted together and imbedded in solder V at the bottom of the casing. A screw N and locknut R provide means of adjustment of the parts. This method of construction makes a rigid column which is not subject to the vibrations common in a laboratory. In practise, the casing is filled with glycerin, which increases the continuity of parts and prevents corrosion of the metallic couple.

The advantages of this design other than those already mentioned are apparent. First, the generous length of the metallic couple insures a maximum of sensitiveness. Second, this sensitiveness is further increased by the mechanical advantage of the lever. Third, continued movement of the bimetallic column in either direction imposes no strain upon any of the parts of the mechanism, a feature not incorporated in thermostats to be found on the market, and one which makes possible accurate control with least adjustment for long and continuous periods of time.

In the construction and testing of this thermostat, the writer is indebted to the New Hampshire College and Experiment Station for the use of laboratories and equipment.

[graphic]
[blocks in formation]

SCIENCE

[blocks in formation]

THE BALANCE, THE STEELYARD AND THE CONCEPT OF FORCE

THE primitive philosophy of Animism, "the doctrine that a great part, if not the whole, of the inanimate kingdom, as well as all animated beings, are endowed with reason, intelligence and volition, identical with that of man," still to a degree sticks in mechanics, in the concept of force. Schopenhauer is quoted as saying:

That the essence of forces in inorganic nature is identical with the will in us, every one believes with full certainty and as a demonstrated truth, who seriously considers it.

R. Eisler says:

Force is a concept which gets its content originally from the capacity of the ego in general by means of its will to bring about something, to overcome a resistance, and is then immediately superposed upon the objects of the external world. ... Since the ego finds limits to its activity in the external world, feels itself hindered by objects, it inevitably interprets the hindrance as the expression and activity of a sort of will-power analogous to itself which things exert against it and by virtue of which they can or do influence other things. . .

E. Mach says that the concept of force is a survival of fetishism; Kirchhoff, in the famous prefix to his Mechanics, acknowledges the value of the older view in the development of the science, and its usefulness in elementary teaching, but takes for himself this higher ground:

I propose as the problem of mechanics, to describe the motions which occur in nature, and, forsooth, to describe them completely and in the simplest way. I will further add that it should deal only with this, to state what the phenomena are, not to determine their causes.

For him the term force " forms only a means of simplifying the forms of expression, i. e., to express in brief phrases equations which with

out the use of this name could only with difficulty be expressed in words."

Believing that the history of a growing concept is sometimes an aid towards a teacher's understanding of his students' difficulties. I have been interested in forming a conjectural reconstruction of the history of this force concept, from the hidden days of pure animatism to the time when a distinct separation between matter and force concepts began to show itself; helping myself meanwhile with such facts as archeology scantily shows us about the most ancient tools, contrivances and ways of life.

To put the problem as a question: When and how was it learned that very different objects may have the same weight? That the same object may have different weights? To treat of force mainly in the weight form is no wrong, on account of the universality of gravitation and the fact that forces even to-day are measured mainly in terms of weight.

The second question is quickly answered; before Richer in 1673 returned to Paris from Cayenne with a report on the going of his clock in the two places, no one had suspected a variability of weight; Huygens concluded from this report that bodies in high latitudes fall faster, and are heavier, than in low; but even now this conclusion remains a deduction from refined instrumental observation; no mason's assistant can say from his personal experience that it is harder to lift a hod of bricks in Edinburgh than in Quito. To us all, the weight of a thing is constant.

That different objects may have the same weight is an extremely ancient idea, so familiar as to be a truism, I dare say, even to the pyramid builders and their forefathers. But I suppose that even truisms were once discoveries; this one, perhaps, became the property of man because he labored.

Assuming that sensations of effort are real, I would classify them, perhaps naïvely, in three groups: Sensations of

(a) Effort proper central, which go with the sending of the nerve message from the central nervous system.

(b) Stress-the nerve message reaches the

muscles, they contract, their changes in form affect the sensory endings of themselves and of neighboring parts, as the skin, the joints, etc., by virtue of arterial and venous compression, the circulation and the breathing also are affected, and, through them, distant parts of the body.

(c) Yielding-changes in stress occur when external bodies give way to the muscles and bones, or when the body itself is moved, as in jumping.

Normally (a) and (b) go together; in nightmare most of us have felt the will paralyzed, the body apparently not responding to the centers; in paralysis the separation may be permanent; I have read that the separation occurs in curare poisoning, when the motor nerves no longer actuate the muscles, but consciousness and sensation remain.

But (c) varies with the object dealt with, and also, for the same object, with bodily health and tone. It varies with the way the object is dealt with. Its variations, combined with the evidence of other sensations, enable us to distinguish between the self and the notself, and between the parts of the not-self, of the external world. With (a) and (b) but without (c) we would know little of the mechanical qualities of bodies. With (c) we get notions of bodies differing not only in color, odor, etc., but also in weight; for to move objects, whether to lift, carry or throw them, requires effort, and the efforts for lifting, carrying and throwing a given body are of the same order of magnitude. Like bodies of about equal extent require like efforts; like bodies of unequal extent require unlike efforts; but equal extent does not condition equal efforts; e. g., a block of wood and a boulder. So we can add to the differing qualities of bodies given by sensations of color, odor, etc., weight and specific heaviness. This effortdemanding quality, varying among bodies and with the condition of the person, would early be abstracted, and the concept weight would appear, in positive (heavy) and comparative (heavier, lighter) degrees. Weight was found to be a quality of solids and liquids universally; the sensations of effort have not yet

made it apparent to us in the case of air, and Galileo first showed it there by experimental means weighing compressed air-which appeal to other senses and to the reason. The savage laborer would have a rough idea of equality in his backloads, he might recognize this equality in backloads of venison or firewood, he might count backloads, bucks or arrows, and so attain crude notions of ratios, and in all things he would perceive the demand for effort, and so recognize the existence of heavy matter of all sorts; the sorts all being alike only in this effort-demanding quality.

Knowing effort only through the sensations of effort, which are subject to Weber's law, and through that form of hysteresis called memory, we can compare efforts, and the weights to which they correspond, only very crudely for equality, practically not at all for ratio, and with diminishing accuracy after longer intervening times. However, efforts being apparently equal, so are weights assumed to be, and, vice versa, bodies of like material and the same size are taken to have equal weights without "hefting them." One rabbit is about as big and so weighs about as much as another.

That two rabbits weigh twice as much as one, however, is not an experience, but a judgment. The effort sensation for two rabbits is not in any sense double that for one; if a man can lift a side of beef with great effort, is the effort required to lift two sides at once twice as great, when he perhaps can not lift the two sides at all? Is the effort made by a stronger man who lifts the two double that of the weaker lifting one?

A very ancient method of bearing loads, dating back to prehistoric times and portrayed in the most ancient records, is the carrying stick or yoke. Convenience and comfort in using this are greatest when the bearer is at the center, which is when equal numbers or volumes of like things swing from the two ends. This, I suppose, led to the invention of the balance with equal arms as a more refined and objective, more "honest," means for the inverse purpose of testing equality in respect to this effort-demanding quality, weight or quan

tity of matter. One Greek name for the balance is vyóv, yoke; but the implement itself dates to measureless antiquity. H. L. Roth,1 quotes Mr. Ivan Chien, of the Chinese Legation in London, to the effect that Chinese history assigns the making of scales to the reign of the Emperor Fu Hi, B. c. 2956. Baumeister (Denkmäler) says it was known in Homeric times; excavations in Crete show that in the recently uncovered civilization of its people the balance was used; Egyptian hieroglyphics show it in ancient use. As the beam was commonly of wood it has not been preserved from those early days.

But why should people desire a more objective, more honest, means of comparing things than by "hefting" or counting? I take it, because of trade, whose routes were marked in Europe even in the Stone Age (as is known from the migration all over the continent of flints of identifiable origin). When the trade in metals grew up, accuracy and standards became of an importance hitherto unprecedented and with them arose the balance and calibrated weights. Lepsius2 is referred to as figuring a sliding weight on a balance beam of ancient Egypt; I have not seen the figure; one would assume that such a sliding weight, serving perhaps as a handy tare, might have suggested the next improvement in weighing apparatus, the steelyard. Whether it did or not must remain for a while unknown; for the only authorities accessible to me are irreconcilably in contradiction as to the date earliest recorded of the Roman steelyard.

There are two forms of steelyard, the Danish and the Roman. The former seems once to have been very common. Sökeland describes a large variety, from simple clubshaped sticks to elaborately worked metal pieces. It was slung by a cord; the unknown weight hung from another cord fixed near one end, and the more or less heavy knobbed or swelling end beyond the fulcrum balanced the unknown. 1 Jour. Roy. Anthrop. Inst., 47, 1912.

2 Denkmäler, III., 39, No. 3.

3 Translated in Smithsonian Annual Report, 1900, p. 551.

In weighing the fulcrum was shifted from place to place, and there were notches for the suspending cord, determined, no doubt, with known weights, these having been calibrated with the balance. This Danish steelyard, desemer or bismar had, then, a graduated beam whose graduations followed no observable law and were wholly empirical. It is this that Aristotle discusses in his "Mechanical Problems," though without much success.

The Roman steelyard, "Statera Romana," familiar in modern form and but little improved since classical antiquity, appeared first perhaps in Egypt, perhaps in Campania. I can only quote authorities.

F. Müller:4

B.C. 1350. The steelyard with running weight is in use among the Egyptians.

L. Darmstaedter :5

B.C. 1400. The steelyard with running weight is in use at the time of the Egyptian king Amenophis IV.

F. M. Feldhaus:"

Unequal armed balance with running weight, usually called Roman steelyard. This balance has a short arm, on which the weighing pan hangs, and a long arm, bearing a graduation and notches for suspending a running weight. The steelyard is known to have been in use in Egypt about B.C. 1400.

Against these very definite statements must be set the authority of Sir J. G. Wilkinson' and of Dr. L. W. King and Flinders Petrie, and of all others, as far as I know, who have published on the subject or answered my inquiries about it, to the effect that the Egyptians did not have the steelyard till the Roman period. Harper's "Book of Facts (1905) says that it is mentioned B.C. 315-I do not know by whom.

[ocr errors]

Incidentally, I may say that I was not a

4''Zeittafeln zur Geschichte der Mathematik,” etc., p. 3 (1892).

5"Handbuch zur Geschichte der Naturwissenschaften,'' etc., p. 3 (1908).

''Die Technik,” p. 1251 (1914).

7''Manners and Customs of the Ancient Egyptians" (1878).

8 Quoted by H. L. Roth, l. c.

little surprised to find this contradiction, and that so well known an instrument of trade should have so uncertain an origin.

I will assume that the Roman steelyard dates back to B.C. 400, and was then known through Mediterranean civilization. He who first graduated it may be called the true discoverer of the law of moment equilibrium, the law of the lever. With any pry or crowbar, or with the bismar, one would have to search for the law deliberately; but this improved weighing apparatus made for trade purposes displays its law to the eye. I imagine the inventor as using a bismar beam, but keeping the fulcrum fixed and sliding along a rider weight, calibrating the beam by means of known balance weights in the pan. The unaided eye could see that equal added weights in the pan corresponded to equal increments of length on the graduation; and so we may understand how Aristotle (B.C. 384322), long before Archimedes (B.C. 287-212), was able to state the law thus "o . . . as the weight moved is to the weight moving it, so, inversely, is the length of the arm bearing the weight to the length of the arm nearer the power...." This he attempts to demonstrate as a consequence of the properties of the circle, but with poor success.

Archimedes, knowing this law of the lever, wrote a book on the subject, unfortunately lost. Another book of his has come down to us, in which he discusses the subject of balanced bodies and the location of centers of gravity in certain plane figures. He does not define center of gravity, but from the use he makes of the term in his demonstrations it is clear that he means by it the point where a body balances when there suspended. This point he treats as representative of the body, and assuming this he attempts a demonstration of the law of the straight horizontal lever, or law of moment equilibrium. E. Mach10 points out, however, that this demonstration, superficially convincing, is seen to be fallacious

"Questiones Mechanicæ," E. S. Forster, trans.

(1913).

10 Science of Mechanics," McCormack trans., p. 18 (1902).

« PreviousContinue »