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April, I92I. ] CURRENT TOPICS. 573 from one part of the variable field to another. He is able to show that his theory is consistent with the inverse square law, with the deflection of light by the sun and with the gravitational effect upon the frequency of light emitted by an atom. " It may be said that since matter is certainly partly electrical and since the refractive index of the ether certainly varies near large masses, it seems certain that part, at least, of the observed gravitational forces must be due to an action of the kind considered in this paper, so that it is satisfactory to find that it is possible to explain the whole attraction by means of this kind of actio'n." G. F. S. The Charge on the Atomic Nucleus and the Law of Force. J. CI~ADWlCK. (Phil. Mag., December, I92O.)--" The theory of the nuclear constitution of the atom, put forward by Sir Ernest Ruth- erford in 191I , has been confirmed by evidence gathered from such various sources that it now forms, the foundation on which the development of atomic physics is based. On this theory the positive charge associated with an atom is concentrated on a massive nucleus of small dimensions, surrounded by a distribu- tion of electrons extending over a distance comparable with the diameter of the atom, as usually understood. " The physical and chemical properties of an element are de- termined by the charge on the nucleus, for this fixes the number and arrangement of the external electrons, on which these prop- erties mainly depend. The mass of the nucleus influences the arrangement of the electrons only to a very small degree. The nuclear charge is thus the fundamental constant of the atom and the question of its actual magnitude of great importance for the development of atomic theory." As the consequences and implications of Rutherford's theory became understood attempts were made to connect the nuclear charge with other atomic constants. " van den Broek suggested that the nuclear charge might be equal to the atomic number of the element, i.e., the number of the element when all the elements are arranged in order of increasing atomic weight." The pahnary significance of the atomic number in this connection was brought forward by the brilliant young British physicist, Moseley, whose untimely death at Gallipoli was the greatest single loss to science inflicted by German aggression. He showed that the X-ray spec- tra of the elements was dependent on the square of a number which became greater by one when passage was made from one element to the element of next higher atomic weight. " On the nuclear theory of atomic structure this characteristic number must be closely connected with the charge on the nucleus, and Moseley concluded that the number gave in fundamental units the actual value of this charge. This is one of the most important generalizations in modern physics, and gives a starting-point for

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Page 1: The charge on the atomic nucleus and the law of force

April , I92I. ] CURRENT TOPICS. 573

f rom one par t of the variable field to another. He is able to show that his theory is consis tent with the inverse square law, with the deflection of l ight by the sun and with the gravi ta t ional effect upon the f requency of light emit ted by an atom. " I t may be said that since ma t t e r is cer tainly par t ly electrical and since the refract ive index of the ether certainly varies near large masses, it seems certain tha t part , at least, of the observed gravi ta t ional forces mus t be due to an action of the kind considered in this paper, so that it is sa t is factory to find tha t it is possible to explain the whole a t t ract ion by means of this kind of actio'n."

G. F. S.

The Charge on the Atomic Nucleus and the L a w of Force. J. CI~ADWlCK. (Phil. Mag., December, I92O.)--" The theory of the nuclear const i tut ion of the a tom, put forward by Sir Ernes t Ruth- erford in 191I , has been confirmed by evidence ga thered f rom such var ious sources tha t it now forms, the foundat ion on which the deve lopment of a tomic physics is based. On this theory the posit ive charge associated with an a tom is concent ra ted on a massive nucleus of small dimensions, sur rounded by a distr ibu- tion of electrons extending over a distance comparab le with the d iameter of the atom, as usual ly understood.

" The physical and chemical proper t ies of an e lement are de- t e rmined by the charge on the nucleus, for this fixes the number and a r r angemen t of the external electrons, on which these prop- erties mainly depend. The mass of the nucleus influences the a r r a n g e m e n t of the electrons only to a very small degree. The nuclear charge is thus the fundamenta l constant of the a tom and the question of its actual magni tude of grea t impor tance for the deve lopment of a tomic theory ."

As the consequences and implicat ions of Ruther ford ' s theory became unders tood a t t emp t s were made to connect the nuclear charge with other a tomic constants . " van den Broek suggested tha t the nuclear charge might be equal to the a tomic n u m b e r of the element, i.e., the num ber of the e lement when all the e lements are a r ranged in order of increasing a tomic weight ." The pahna ry significance of the a tomic num ber in this connection was b rought forward by the bril l iant young Brit ish physicist , Moseley, whose un t imely death at Gallipoli was the grea tes t single loss to science inflicted by German aggression. H e showed that the X- ray spec- tra of the e lements was dependent on the square of a number which became grea ter by one when passage was made f rom one e lement to the e lement of next higher a tomic weight . " On the nuclear theory of a tomic s t ruc ture this character is t ic n u m b e r mus t be closely connected with the charge on the nucleus, and Moseley concluded that the number gave in fundamenta l units the actual value of this charge. This is one of the most impor tan t genera l iza t ions in modern physics, and gives a s tar t ing-point for

Page 2: The charge on the atomic nucleus and the law of force

574 CURRENT TOPICS. [J. F. I.

the deve lopment of the external s t ruc ture of the a tom." The only direct method of measu r ing the charge on the nucleus is by s tudy ing the single sca t te r ing of alpha particles. W h e n a pencil of these falls on a thin sheet of mat ter , the number of the scat- tered part icles fal l ing per second on a unit area of screen at a known distance and angle with the pencil is connected with the num- ber of particles per second in the pencil by a fo rmula in which every quan t i ty is ei ther a known cons tan t or a measurab le quan- t i ty except the nuclear charge of the sca t te r ing a toms. This charge can therefore be calculated f rom the formula, when the resul ts of exper iment are inserted in it.

The direct as well as the scat tered alpha part icles were counted by the scinti l lat ions they produced upon the same zinc sulphide screen. If there were th i r ty scat tered part icles per minute , there would be about 2o,ooo direct part icles in the same time. To count this large n u m b e r a ro ta t ing disk wi th a slit was inter- posed in the pa th of the pencil before i t reached the screen, so tha t only a known fract ion of the part icles could pass. Thus the n u m b e r to be observed was made so small that it could readily be counted.

Expe r imen t s were made for three metals , p la t inum, silver and copper. In all cases the part icles counted numbered some thou- sands. N means the n u m b e r by which the fundamenta l charge of electrici ty, the charge of the electron, mus t be mult ipl ied in order to get the nuclear charge of an a tom of the metal.

Atomic Number Metal. N. of Metal .

Platinum . . . . . . . . . . . . . . . . . . . . . . . . 77.4 78 Silver . . . . . . . . . . . . . . . . . . . . . . . . . . . 46.3 47 Copper . . . . . . . . . . . . . . . . . . . . . . . . . . 29.3 29

The a tomic n u m b e r of the meta l is derived f rom its X- ray spec- tra, while N comes f rom the exper iment . The ag reemen t is strik- ing and Mose ley ' s conclusion is confirmed in a r emarkab le way. An examina t ion of fur ther exper imenta l da ta leads to the conclu- sion tha t the inverse square law holds t rue in the region of inves- t igat ion, i.e., within one hundred-bi l l ionth of a cent imeter f rom the nucleus.

G. F. S.

L ime N i t r o g e n . r a T h e claim has been made tha t l ime ni t rogen or commerc ia l calcium cyanamide produces injuries of the skin and of the resp i ra to ry tract, acts as a poison, and gives rise to a disease wi th character is t ic s y m p t o m s - - " l ime n i t rogen disease." SIEBNER (Chemiker Zeitung, I92o , xliv, 369-37 o, 382-383) has made an e labora te s tudy of the subject , and draws the fol lowing conclus ions: The injuries to the skin are due to free caustic l ime which occurs in the cyanamide dust; the injuries to the resp i ra to ry t rac t are exact ly the same as those produced by any dust. Cal-