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JIPMER 2017
Exam
JIPMER
Year
2017
Subject
Physics
Chapter
Nuclear Physics

JIPMER 2017 · Physics · Nuclear Physics

Radioactive decay will occur as follows aligned & _ 86 ^ 220 Rn _...

Radioactive decay will occur as follows 86220Rn⟶84216PO+24He Half life =55s84816Po⟶82212Pb+24He Half life =0⋅66s82212BL+λ∘e Half life =10⋅6h\begin{aligned} & { }_{86}^{220} \mathrm{Rn} \longrightarrow{ }_{84}^{216} \mathrm{PO}+{ }_2^4 \mathrm{He} \text{ Half life }=55 \mathrm{ s} \\ & { }_{84}^{816} \mathrm{Po} \longrightarrow{ }_{82}^{212} \mathrm{ Pb}+{ }_2^4 \mathrm{He} \text{ Half life }=0 \cdot 66 \mathrm{ s} \\ & { }_{82}^{212} \mathrm{BL}+\lambda^{\circ} e \text{ Half life }=10 \cdot 6 \mathrm{ h} \end{aligned} If a certain mass of radon (Rn=220)(R n=220) is allowed to decay in a certain container; then after 5 minutes the element with the greater mass will be

Options

  1. Aradon
  2. Bpolonium
  3. Clead
  4. Dbismuth

Correct answer

C. lead

Step-by-step solution

Let M0M_0 be initial mass of Rn−220R n-220 Number of half-lives of Rn in 5 minutes =5min55s=5×6055≈5.5\begin{aligned} & \text{ Number of half-lives of } R n \text{ in } 5 \text{ minutes }=\frac{5 \mathrm{ min}}{55 \mathrm{ s}} \\ & =\frac{5 \times 60}{55} \approx 5.5 \end{aligned}∴\therefore Mass of Rn−220R n-220 (left) =(12)5.5M0=M045∴=\left(\frac{1}{2}\right)^{5.5} M_0=\frac{M_0}{45} \therefore The mass converted into Po -216 is (44/45) M0M_0, Number of half-lives of Po−216P o-216 in 5 minutes =5min0.66=3000.66≈455∴=\frac{5 \mathrm{ min}}{0.66}=\frac{300}{0.66} \approx 455 \therefore Mass of Po−216P o-216 left =(12)455×4445M0⟶0=\left(\frac{1}{2}\right)^{455} \times \frac{44}{45} M_0 \longrightarrow 0 This means that Po−216P o-216 formed will soon decay to lead. Hence, lead will have maximum mass nearly \left(\frac{44}{45}\right)$ M_0
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