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CHAPTER IV. NATURE OF THE RADIATIONS.

the secondary rays from different radiators is not very different, with the exception of substances such as granite, brick, and cement, which give out secondary rays of nearly twice the penetrating power of other substances.

β and γ rays.

RadiatorDensitySecondary RadiationSec. Rad. / DensityAluminium ·085 cm. λ
Mercury13·614710·8
Lead11·414112·418·5
Copper8·8799·020
Brass8·4819·621
Iron (wrought)7·8759·620
Tin7·4739·920·3
Zinc7·07911·3
Granite2·75420·012·4
Slate2·65320·412·1
Aluminium2·64216·124
Glass2·54417·624
Cement2·44719·613·5
Brick2·24922·313·0
Ebonite1·13229·126
Water1·02424·021
Ice·922628·2
Paraffin solid·91718·821
„ liquid·851618·8
Mahogany·5621·438·223
Paper·4?21·05222
Millboard·4?19·44820·5
Papier-mâché...21·9
Basswood·3620·75722
Pine·3521·86221
X ray screen75·223·6

The secondary radiation not only comes from the surface of the radiator but from a considerable depth. The amount of secondary rays increases with the thickness of the radiator, and, in the case of glass and aluminium,

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