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the astonishing statement in the same article that most of these so-called gravel implements of Europe are doubtless the rejects of manufacture," pre-historic archæologists, and especially those of Europe, will draw their own inferences as to the qualifications for pronouncing an ex cathedra decision of the man who made the statement (Science, Nov. 25, 1892) that "there is not in the museums of Europe or America a single piece of flaked stone found in place in the gravels of America and satisfactorily verified that can with absolute safety be classified as an implement at all."

I have had occasion elsewhere to refer to Mr. Holmes's fondness for making startling assertions, instancing his statement about the Indians, in the same article in Science, that their “quarrying was accomplished mainly by the aid of stone, wood and bone utensils, aided in some cases perhaps by fire. With these simple means the solid beds of rock were penetrated to depths often reaching twenty-five feet."

The readers of Science have lately had an opportunity of observing also that Mr. Holmes "strongly deprecates personalities in scientific discussion." HENRY W. HAYNES.

Boston, March 30.

BOOK-REVIEWS.

The History and Theory of Money. By SIDNEY SHERWOOD. Philadelphia, J. B. Lippincott Co. $2.

THIS book contains twelve lectures delivered in the university extension course at Philadelphia last year before a company of bankers and others interested in the subject of finance Half the lectures are professedly historical and the other half theoretical; but the historical element is really predominant throughout them all. This seems to us a mistake, for the history of money cannot be properly understood nor appreciated without a previous acquaintance with the theory, and in these lectures the theory is not stated with anything like the clearness and fulness which

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the subject demands. However, it was expected that the attendants on the lectures would read and study for themselves during the progress of the course, the books recommended for their use being named in this volume; and such reading would supplement the instruction given in the lectures. Mr. Sherwood, who is attached to the Wharton School of Finance in the University of Pennsylvania, shows a thorough familiarity with his subject, and, what is quite as important, he has no hobbies to ride, and is not prone to extreme or one-sided views. He begins by showing what money is for, what purposes it fulfils in the world's economy, and then proceeds to treat of the different kinds of money in use, with remarks on coinage, on the history of the precious metals, and on government notes and bank notes, with brief discussions of some of the many economic questions which those subjects involve. The lectures are expressed in a plain and straightforward style, which the hearers could readily understand, and they were evidently enjoyed by those who listened to them. For our part, however, we have found the discussions at the end of each lecture, and which are here reported in brief, the most interesting part of the book as well as the most suggestive. There were many persons in the audience well equipped with both theoretical and practical knowledge of the subject, and their discussions with Mr. Sherwood and with one another called up many points that were not touched upon in the lectures, and presented various and sometimes conflicting views. Among the debaters was a lady of socialistic proclivities, whose remarks and questions added variety and piquancy to the scene, though she did not appear to have many sympathizers. On the whole, though it cannot be regarded as an adequate scientific treatisen money, this book will certainly have an interest for all who care for its subject.

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to produce the electrical action on which the first patent rests. The third claim is for the use in such instruments of a diaphragm, made of a plate of iron or steel, or other material capable of inductive action; the fifth, of a permanent magnet constructed as de scribed with a coil upon the end or ends

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box as described; the seventh, of a speaking or hearing tube as described for conveying the sounds; and the eighth, of a permanent magnet and plate combined. The claim is not for these several things in and of themselves, but for an electric telephone in the construction of which these things or any of them are used."

This Company also owns Letters-Patent No. 463,569, granted to Emile Berliner, November 17, 1891, for a combined Telegraph and Telephone, and controls Letters-Patent No. 474,231, granted to Thomas A. Edison, May 3, 1892, for a Speaking Telegraph, which cover fundamental inventions and embrace all forms of microphone transmitters and of carbon telephones.

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NEW METHOD OF PROTECTING BUILDINGS FROM LIGHTNING. SPARE THE ROD AND SPOIL THE HOUSE ! Lightning Destroys. Shall it be Your House or a Pound of Copper?

PROTECTION FROM LIGHTNING.

What is the Problem?

IN seeking a means of protection from lightning-discharges, we have in view two objects, the one the prevention of damage to buildings, and the other the prevention of injury to life. In order to destroy a building in whole or in part, it is necessary that work should be done; that is, as physicists express Ir, energy is required. Just before the lightning-discharge takes place, the energy capable of doing the damage which we seek to preveut exists in the column of air extending from the cloud to the earth in some form that makes it capable of appearing as what we call electricity. We will therefore call it electrical energy. What this electrical energy is, it is not necessary for us to consider in this place; but that it exists there can be no doubt, as it manifests itself in the destruction of buildings. The problem that we have to deal with, therefore, is the conversion of this energy into some other form, and the accomplishment of this in such a way as shall result in the least injury to property and life.

Why Have the Old Rods Failed?

When lightning-rods were first proposed, the science of energetics was entirely undeveloped; that is to say, in the middle of the last century scientifle men had not come to recognize the fact that the different forms of energy — heat, electricity, mechanical power, etc.-were convertible one Into the other, and that each could produce just so much of each of the other forms, and no more. The doctrine of the conservation and correlation of energy was first clearly worked out in the early part of this century. There were, however, some facts known in regard to electricity a hundred and forty years ago; and among these were the attracting power of points for an electric spark, and the conducting power of metals. Lightning-rods were therefore introduced with the idea that the electricity existing in the lightning-discharge could be conveyed around the building which it was proposed to protect, and that the building would thus be saved.

The question as to dissipation of the energy Involved was entirely ignored, naturally; and from that time to this, in spite of the best endeavors of those interested, lightning-rods constructed in accordance with Franklin's principle have not furnished satisfactory protection. The reason for this is apparent when it is considered that the electrical energy existing in the atmosphere Sefore the discharge, or, more exactly, in the column of dielectric from the cloud to the earth, above referred to, reaches its maximum value on the surface of the conductors that chance to be within the column of dielectric; so that the greatest display of energy will be on the surface of the very lightningrods that were meant to protect, and damage results, as so often proves to be the case.

It will be understood, of course, that this display of energy on the surface of the old lightning-rods is aided by their being more or less Insulated from the earth, but in any event the very existence of such a mass of metal as an old lightning-rod can only tend to produce a disastrous dissipation of electrical energy upon its surface," to draw the lightning," as it is so commonly put.

Is there a Better Means of Protection?

Having cleared our minds, therefore, of any idea of conducting electricity, and keeping clearly in view the fact that in providing protection against lightning we must furnish some means by which the electrical energy may be harmlessly dissipated, the question arises, "Can an improved form be given to the rod, so that it shall ald in this dissipation?"

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As the electrical energy involved manifests itself on the surface of conductors, the Improved rod should be metallic; but, instead of making a large rod, suppose that we make it comparatively small in size, so that the total amount of metal running from the top of the house to some point & little below the foundations shall not exceed one pound. Suppose, again, that we introduce numerous Insulating joints in this rod. We shall then have a rod that experience shows will be readily destroyed-will be readily dissipated when a discharge takes place; and it will be evident, that, so far as the electrical energy is consumed in doing this, there will be the less to do other damage.

The only point that remains to be proved as to the utility of such a rod is to show that the dissipation of such a conductor does not tend to injure other bodies in its immediate vicinity. On this point I can only say that I have found no case where such a conductor (for instance, a bell wire) has been dissipated, even If resting against a plastered wall, where there has been any material damage done to surrounding objects.

Of course, it is readily understood that such an explosion cannot take place in a confined space without the rupture of the walls (the wire cannot be boarded over); but in every case that I have found recorded this dissipation takes place just as gunpowder burns when spread on a board. The objects against wolch the conductor rests may be stained, but they are not shattered, I would therefore make clear this distinction between the action of electrical energy when dissipated on the surface of a large conductor and when dissipated on the surface of a comparatively small or easily dissipated conductor. When dissipated on the surface of a large conductor, a conductor so strong as to resist the explosive effect, - damage results to objects around. When dissipated on the surface of a small conductor, the conductor goes, but the other objects around are saved

A Typical Case of the Action of a Small Conductor. Franklin, in a letter to Collinson read before the London Royal Society, Dec. 18, 1755, describing the partial destruction by lightning of a church-tower at Newbury, Mass, wrote, "Near the bell was fixed an iron hammer to strike the hours; and from the tail of the hammer a wire went down through a small gimlet-hole in the floor that the bell stood upon, and through a second floor in like manner; then horizontally under and near the plastered ceiling of that second floor, till it came near a plastered wall; then down by the side of that wall to a clock, which stood about twenty feet below the bell. The wire was not bigger than a common knitting needle. The spire was split all to pieces by the lightning, and the parts flung in all directions over the square in which the church stood, so that nothing remained above the bell. The lightning passed between the hammer and the clock in the above-mentioned wire, without hurting either of the floors, or having any effect upon them (except making the gimlet-holes, through which the wire passed, a little bigger), and without hurting the plastered wall, or any part of the building, so far as the aforesaid wire and the pendulum-wire of the clock extended; which latter wire was about the thickness of a goose-quill. From the end of the pendulum, down quite to the ground, the building was exceedingly rent and damaged. . . . No part of the aforementioned long, small wire, between the clock and the hammer, could be found, except about two inches that hung to the tall of the hammer, and about as much that was fastened to the clock; the rest being exploded, aud its particles dissipated in smoke and air, as gunpowder is by common fire, and had only let a black smutty track on the plastering, three or four inches broad, darkest the middle, and fainter towards the edges, all along the ceiling, under which it passed, and down the wall." One hundred feet of the Hodges Patent Lightning Dispeller (made under patents of N. D. C. Hodges, Editor of Science) will be mailed, postpaid, to any address, on receipt of five dollars ($5).

Correspondence solicited. Agents wanted. AMERICAN LIGHTNING PROTECTION CO., 874 Broadway, New York City.

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RACES AND PEOPLES.

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SCIENCE

NEW YORK, APRIL 21, 1893.

LABORATORY INSTRUCTION IN PHYSICS.

BY D. W. HERING, UNIVERSITY OF THE CITY OF NEW YORK.

THERE are various practices, and seemingly but two clearly defined methods of teaching physics in college laboratories. The first method, which may be called the progressive one, treats the general subject of physics by going through its various divisions successively, until the whole ground has been covered, whether thoroughly or superficially. For students who have had no preliminary training in physics, this method is the only practicable one if they are to begin their study in the laboratory. The other may be called the method of analysis. It assumes that the pupil has received a fair course of instruction in the principles of the science before he enters upon laboratory work. Then it is a matter of indifference whether his first exercise is one in optics. or in electricity; in radiation, or in specific gravities. He will examine a body of any sort with reference to its various properties, taking account of as many as he can, which in some instances may embrace nearly the whole range of physics. This method then does not present the different features of physics so much as the physical features of different things.

At first sight it would appear as if the method that is pursued for the direct purpose of learning the science would be the one best fitted to give an acquaintance with it, and perhaps this would be true if sufficient time could be given to it to deal with the various branches of physics with tolerable thoroughness, but laboratory work by an untrained pupil is slow at best, and time is limited. It is important, therefore, to follow the plan that will give good results without loss of time.

If physics as a science were distinctly progressive in its nature, one step being essential to a comprehension of the next, and therefore of necessity a preliminary to it, there could be no question as to the best order of proceeding in teaching or in learning the subject. There would still be room for question as to how much should be done by the teacher in experimental illustration with discussions, before putting the pupil to experimenting on his own account, but the order of dealing with the subject in any case would be determined beforehand. But it is thus progressive to only a limited degree. Except for the principles of mechanics, which permeate the entire science, physics, in all its diversity, may be dealt with regardless of the order in which the subjects are taken up And this exception is not always recognized. Among recent standard text-books which are meant to be especially adapted to laboratory practice, but which mean to omit none of the elementary principles of physics, there is every variety in arrangement of topics. One begins with specific gravity and air pressure, follows with dynamical principles, and presents light as the final subject. Another begins with magnetism, introduces the last third of the work by dynamics, and closes with sound. Still another begins with properties of matter and dynamics and ends with light; while a fourth begins with the mechanical powers and closes with magnetism and electricity. Even the special divisions, as electricity, for example, can scarcely be said to be developed from one principle that necessarily comes first, to another that can be reached only at the end of a well-defined series. Some classification of topics can always be made, but the tendency to-day is to diminish rather than increase the number of classes. Considerations of intrinsic difficulty, or length of time that can be given without interruption, or the season of the year when sunny days may be expected, or other special points may lead to a preference as to the order of subjects, but there is little in the nature of the subjects themselves to determine it.

ures.

The status of the student when he is to enter upon the work which this paper is to discuss, will depend upon the manner in which he obtained his first training in physics. He may have acquired his early knowledge by experimentation from the beginning, or he may have been taught from descriptive text-books supplemented by experimental lectures from the teacher, or he may have had a combination of both. In the first case, he had to find out principles and laws as well as (to him) disconnected facts by his own experimentation; in the second, he has been made acquainted with the leading laws and properties and perhaps has had some opportunity to verify and apply them. Whether an attempt to learn physics from the beginning by practice is profitable or advisable has been much discussed, and it is outside of our purpose to enter upon that question. It is a plan that has grown in favor greatly of late, and has been insisted upon by Harvard College, as a preparation for those who are to pursue the subject in college. Let us suppose the pupil to have acquired a general, though elementary, acquaintance with the principles of the science, that he has reached the standard of at least a well-prepared college junior. For this he has probably been called upon to cover the whole range of the subject whether by experiment, or by recitations and experimental lectThe advocates of the two methods of preparation will find points to offset one another in the results attained. The experimental student will have acquired his knowledge in a very valuable way, by objective study, by the inductive method. He will have learned to do by doing." This has become a favorite idea with educators in almost every branch of learning, and its advantages are undeniable in most lines of work, but they are not equally great or equally obvious in all branches or at all stages. It is a most effective way so far as it goes, but in physics the experiments concerning any one point, or involving any law, will have been so small in number under the best opportunities, that the student must infer the law from instances altogether too few and too little varied, to justify an inference. Potent as the inductive method has been in science, its demonstrations are never incontestable, they never rise above a moral certainty, and do not even approach it, if the instances upon which the conclusions are based are not numerous, or else very accurate. The student will in reality have done nothing more than illustrate a point, doing in a crude way what the lecturer before a large class does in a better way. Still the experiment and its results will impress themselves upon him because he did the work himself. In this he will have the advantage of the lecture-taught student. The knowledge of the latter, however, is likely to be more correct as to principles. On the whole, the two classes may be said to approach the higher laboratory practice about equally well equipped: the former better prepared for manipulation with perhaps less readiness to appreciate the science; the latter better prepared to discriminate as to principles, but less expert in determining them. Didactic and experimental instruction are now so well combined in some secondary schools as to make their work superior to that offered in many colleges. Having been fairly well taught by any method, we may suppose the student ready for practical work somewhat more advanced than is to be had in secondary schools, or even in the general course of physics in an average American college. What plan shall be followed in his laboratory work? Presumably that plan is best which is best fitted to accomplish its purpose. What is the purpose of his work? Usually not independent research or original investigation. Work of that class is generally undertaken only by graduates or special students, who are not obliged to accomplish a definite amount in a given time. The higher laboratory work of the college undergraduate is for the purpose of making him practically familiar with physical laws, not in one particular

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