1
~une, 1920.] CURRENT TOPICS. 8I 5 Distribution of the Chemical Elements.--Geochemists have calculated the percentage by weight of the different elements in the known crust 0¢ the earth, including the rocks, water, and atmosphere. INGO W. D, HACKH (Science Progress, I920, xiv, 6o2-6o7) has used these figures as the basis of his calculations. If the per cent. of each element, which is present, be divided by its atomic weight, the quotient shows the relative proportion of its atoms in the crust. Of the 25 elements, whose atoms are most abundant, those of bromine are least abundant; and the relative proportion of bromine atoms was therefore taken as unity; the other elements then fell into the following order of magnitude with respect to the occurrence of their atoms : O .... 249,850 Mg... 6,835 Ti ...... 714 N ...... I7r V ........ 23 H .... 75,312 Ca .... 6,422 C1...... 45I Mn ..... II6 Li ....... 22 Si .... 72,86o Fe .... 5,982 F ....... 421 Ba ...... 46 Sr ....... i6 A1 .... 21,528 K ..... 4,660 P ....... 283 Cr ...... 46 Zr ....... 13 Na... 8,2oo C ..... I,I99 S ....... 274 Ni ...... 26 Br ....... I Hydrogen thus follows directly after oxygen wit,. the relative occurrence o~ its atoms. :pect to J. s. H. The Dissipation of Heat by Various Surfaces in Still Air. T. S. TAYLOR. (Phys. Rez,., March, I92O.)--Three vessels of sheet tin, IO era. in diameter and 5° cm. long, were made. One was left bare, one was covered closely with sheet asbestos 0.33 ram. thick and the third was covered loosely with the same material. All three were filled with hot water and allowed to cool under similar conditions. The result was obtained that the bare vessel lost only 7° per cent. as much heat per minute as the loosely covered one and 63 per cent. as much as the tightly covered vessel. The effect of dusting the sur- face with coal ashes was to slightly increase the radiation from the bare surface and to diminish to a somewhat greater extent the loss from the tightly covered vessel. G. F. S. Variation of Transparency to Total Radiation with Tempera- ture of Source. S. L. BRowx. (Phys. Rev., March, I92O , p. 217.)- Glass, rock salt, mica, celluloid and paraffin were examined. In all the transparency for total radiation increased markedly as the tem- perature of the radiating body rose from 2oo ° to 12oo ° C. For glass the amount transmitted at the lower temperature was 5.8 per cent. and at the higher 61 per cent. For rock salt the corresponding num- bers are 35 and 5o.5. Glass alone shows a departure from the general rule by having a minimum transmission at 3oo °. Whether heated or cooled from this temperature its transmission increases. G. F. S.

The dissipation of heat by various surfaces in still air

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Page 1: The dissipation of heat by various surfaces in still air

~une, 1920.] CURRENT TOPICS. 8I 5

D i s t r i b u t i o n of the Chemica l E l e m e n t s . - - G e o c h e m i s t s have ca l cu la t ed the p e r c e n t a g e by w e i g h t of the d i f fe ren t e l e m e n t s in the k n o w n c rus t 0¢ the ear th , i n c l u d i n g the rocks, water , and a tmosphe re . INGO W. D, HACKH (Science Progress, I920, xiv, 6o2-6o7) has used these f igures as the basis of his ca lcu la t ions . If the per cent . of each e lement , wh ich is p resen t , be d iv ided by i ts a tomic we igh t , the q u o t i e n t shows the re la t ive p r o p o r t i o n of i ts a t oms in the crust . Of the 25 elements, whose atoms are most a b u n d a n t , those of b r o m i n e are leas t a b u n d a n t ; and the re la t ive p r o p o r t i o n of b r o m i n e a toms was therefore t a ke n as u n i t y ; the o the r e l e m e n t s t hen fell in to the fo l l owing order of m a g n i t u d e w i th respect to the occu r r ence of the i r a t oms :

O . . . . 249,850 M g . . . 6,835 Ti . . . . . . 714 N . . . . . . I7r V . . . . . . . . 23 H . . . . 75,312 Ca . . . . 6,422 C1 . . . . . . 45I Mn . . . . . II6 Li . . . . . . . 22 Si . . . . 72,86o Fe . . . . 5,982 F . . . . . . . 421 Ba . . . . . . 46 Sr . . . . . . . i6 A1 . . . . 21,528 K . . . . . 4,660 P . . . . . . . 283 Cr . . . . . . 46 Zr . . . . . . . 13 Na. . . 8,2oo C . . . . . I,I99 S . . . . . . . 274 Ni . . . . . . 26 Br . . . . . . . I

H y d r o g e n thus fol lows d i rec t ly af ter o x y g e n wit , . the re la t ive occu r rence o~ i ts a toms .

:pect to

J. s. H.

The Dissipation of Heat by Various Surfaces in Still Air. T. S. TAYLOR. (Phys. Rez,., March, I 9 2 O . ) - - T h r e e vessels of sheet tin, IO era. in diameter and 5 ° cm. long, were made. One was left bare, one was covered closely with sheet asbestos 0.33 ram. thick and the third was covered loosely with the same material . All three were filled with hot water and allowed to cool under similar conditions. The result was obtained that the bare vessel lost only 7 ° per cent. as much heat per minute as the loosely covered one and 63 per cent. as much as the tightly covered vessel. The effect of dust ing the sur- face with coal ashes was to slightly increase the radia t ion f rom the bare surface and to diminish to a somewhat greater extent the loss f rom the tightly covered vessel.

G. F. S.

Variation of Transparency to Total Radiation wi th T e m p e r a - tu re of Source. S. L. BRowx. (Phys. Rev., March, I92O , p. 217.)- Glass, rock salt, mica, celluloid and paraffin were examined. In all the t ransparency for total radiat ion increased markedly as the tem- pera ture of the rad ia t ing body rose f rom 2oo ° to 12oo ° C. For glass the amount t ransmi t ted at the lower tempera ture was 5.8 per cent. and at the higher 61 per cent. F o r rock salt the cor responding n u m - bers are 35 and 5o.5. Glass alone shows a depar ture f rom the general rule by having a m i n i m u m t ransmiss ion at 3oo °. W h e t h e r heated or cooled f rom this t empera tu re its t ransmiss ion increases.

G. F. S.