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CHAPTER XI. TRANSFORMATION PRODUCTS OF RADIUM.

may be of interest to mention that the writer calculated the period of radium F by a similar method, before its value was experimentally determined, and found that F should be half transformed in about one year. This is not very different from the experimental value of 143 days found later. In addition, it was assumed in the calculation that the α particles from C and F were projected with the same velocity, and in consequence produced the same amount of ionization. In practice, however, it is found that the α particle of F is absorbed in about half the distance of the α particles of C, and in consequence produces only about half of the ionization of the latter. If this correction were made, the calculated period for half transformation would be six months instead of one year.

A table of the transformation products of radium, together with some of their physical and chemical properties, is given below.

Transformation ProductsTime to be half transformedRaysChemical and Physical Properties
Radium1200 yearsα rays
Emanation3·8 daysα raysChemically inert gas; condenses at -150° C.
Radium A (active deposit of rapid change)3 mins.α raysBehaves as solid; deposited on the surface of bodies; concentrated on cathode in electric field. Soluble in strong acids; volatile at a white heat. B is more volatile than A or C.
:: B (same)21 mins.no raysSame
:: C (same)28 mins.α, β, γ raysSame
:: D (active deposit of slow change)about 40 yearsno raysSoluble in strong acids and volatized below 1000° C.
:: E (same)6 daysβ (and γ)Non-volatile at 1000°C.
:: F (same)143 daysα raysVolatile at 1000° C; deposited from solution on to bismuth plate.
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236. Variation of the activity over long periods of time. We are now in a position to calculate the variation of the α and β ray activity of the active deposit over long periods of time. If it is supposed that the matter initially deposited consists only of D, the amounts P, Q and R of radium

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