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Concepts Of Physics MCQ Edition [Volume 2]
Exam
Concepts Of Physics MCQ Edition [Volume 2]
Subject
Physics
Chapter
The Nucleus

Concepts Of Physics MCQ Edition [Volume 2] · Physics · The Nucleus

In a nuclear physics experiment, radioactive isotopes are produced...

In a nuclear physics experiment, radioactive isotopes are produced at a constant rate dN/dt=RdN/dt = R. A series circuit is formed by connecting an inductor of inductance 100 mH100 \text{ mH}, a resistor of resistance 100Ω100 \Omega, and a battery. The circuit is switched on at the exact instant the production of the radioactive isotope begins. It is observed that the ratio i/Ni/N remains constant over time, where ii represents the current in the circuit at time tt and NN represents the number of active nuclei at time tt. Determine the half-life of the isotope.

Options

  1. A6.93×10−4 s6.93 \times 10^{-4} \text{ s}
  2. B693 s693 \text{ s}
  3. C0.693 s0.693 \text{ s}
  4. D1.0×10−3 s1.0 \times 10^{-3} \text{ s}

Correct answer

A. 6.93×10−4 s6.93 \times 10^{-4} \text{ s}

Step-by-step solution

The rate of change of the number of active nuclei is given by dNdt=R−λN\dfrac{dN}{dt} = R - \lambda N, where RR is the constant production rate and λ\lambda is the decay constant.

Integrating with the initial condition N(0)=0N(0) = 0, we get N(t)=Rλ(1−e−λt)N(t) = \dfrac{R}{\lambda}(1 - e^{-\lambda t}).

For the series LR circuit, the current at time tt is given by i(t)=i0(1−e−RresLt)i(t) = i_{0}(1 - e^{-\frac{R_{res}}{L}t}), where RresR_{res} is the resistance and LL is the inductance.

Given that the ratio i(t)N(t)\dfrac{i(t)}{N(t)} is constant over time, the exponential terms must be identical. Thus, λ=RresL\lambda = \dfrac{R_{res}}{L}.

Substituting the given values Rres=100ΩR_{res} = 100 \Omega and L=100 mH=0.1 HL = 100 \text{ mH} = 0.1 \text{ H}:

λ=1000.1=1000 s−1\lambda = \dfrac{100}{0.1} = 1000 \text{ s}^{-1}

The half-life of the isotope is T1/2=ln⁡2λ=0.6931000=6.93×10−4 sT_{1/2} = \dfrac{\ln 2}{\lambda} = \dfrac{0.693}{1000} = 6.93 \times 10^{-4} \text{ s}.
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