(a) The emission of this sign at the start can be calculated as:
R=λN0=t1/20.693N0=t1/20.693Mmolarm0NA
From there, we know that R = 15 Ci (1 Ci = 3.70 X 1010 Bq= 3.70 X 1010 decays/s), and that for 3H the molar mass Mmolar=3.016 g/mol and the half-time for the β-decay t1/2 = 12.43 years:
R=t1/20.693Mmolarm0NA⟹m0=0.693NAt1/2⋅R⋅Mmolar
m0=0.693(6.022×1023atoms/mol)(12.43years(1year3.156×107s))(15Ci(1Ci3.70×1010Bq)(1Bq1atom/s))(3.016g/mol)
m0=0.693(6.022)(12.43)(3.156)(15)(3.70)(3.016)×107+10−23g of 3H
m0=1573.47×10−6g of 3H=1.573×10−3g of 3H
(b) After five years, we can calculate the mass by using:
m(t)=m0e−λt=m0e−t1/20.693t
We substitute m0 as the start mass calculated before and t=5 years to find:
m(t=5 years)=(1.573×10−3g)e−(12.43years5years)(0.693)
m(t=5 years)=(1.573mg)e−12.43(5)(0.693)=(1.573mg)e−0.278761...
m(t=5 years)=(1.573mg)(0.75672)=1.190mg of 3H
In conclusion, we find that (a) the initial mass of 3H on the sign is m0=1.573 mg and (b) after five years the mass decreases to m(5 years)=1.190 mg of the 3H isotope that has a β-decay.
Reference:
- Young, H. D., & Freedman, R. A. (2015). University Physics with Modern Physics and Mastering Physics (p. 1632). Academic Imports Sweden AB.
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