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QJEEAdv18Ph6653: JEE Advanced 2018 Physics - Class 11 JEEAdv18Ph6653 Solution: If the measurement errors in all the independent quantities are …

If the measurement errors in all the independent quantities are known, then it is possible to determine the error in any dependent quantity. This is done by the use of series expansion and truncating the expansion at the first power of the error. For example, consider the relation z=x/y.z = x/y. If the errors in x,yx,y and zz are Δx,Δy\Delta x,\Delta y and Δz,\Delta z, respectively, then
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The series expansion for (1±Δyy)−1,{\left( {1 \pm {{\Delta y} \over y}} \right)^{ - 1}}, to first power in Δy/y.\Delta y/y. is 1±(Δy/y).1 \pm \left( {\Delta y/y} \right). The relative errors in independent variables are always added. So the error in zz will be
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The above derivation makes the assumption that \Delta x/x &lt; &lt; 1, \Delta y/y &lt; &lt; 1. Therefore, the higher powers of these quantities are neglected.

In an experiment the initial number of radioactive nuclei is 3000.3000. It is found that 1000±401000 \pm 40 nuclei decayed in the first 1.0s.1.0s. For \left| x \right| &lt; &lt; 1. ln⁡(1+x)=x\ln \left( {1 + x} \right) = x up to first power in x.x. The error Δλ,\Delta \lambda , in the determination of the decay constant λ,\lambda , in s−1,{s^{ - 1}}, is

Multiple Choice Options

  • A 0.040.04
  • B 0.030.03
  • C 0.020.02
  • D 0.010.01

Step-by-Step Verified Solution

The law of radioactive decay gives number of undecayed nuclei N at time t as N=N0e−λtN = {N_0}{e^{ - \lambda t}} , where N0 is number of nuclei at t = 0 and λ\lambda is the decay constant. The number of nuclei decayed till time t is given by Nd=N0−N{N_d} = {N_0} - N . Thus, the decay constant is given by

λ=1tln⁡N0N=1tln⁡N0N0−Nd\lambda = {1 \over t}\ln {{{N_0}} \over N} = {1 \over t}\ln {{{N_0}} \over {{N_0} - {N_d}}} .

Since, N0 = 3000 and t = 1 s are given without any error, we assume that error in λ\lambda is due to error in Nd only. Hence, we can write above equation as

λ+Δλ=1tln⁡N0N0−(Nd+ΔNd)\lambda + \Delta \lambda = {1 \over t}\ln {{{N_0}} \over {{N_0} - ({N_d} + \Delta {N_d})}}

=1tln⁡N0(N0−Nd)(1−ΔNd/(N0−Nd))= {1 \over t}\ln {{{N_0}} \over {({N_0} - {N_d})(1 - \Delta {N_d}/({N_0} - {N_d}))}}

=1tln⁡N0N0−Nd−1tln⁡(1−ΔNdN0−Nd)= {1 \over t}\ln {{{N_0}} \over {{N_0} - {N_d}}} - {1 \over t}\ln \left( {1 - {{\Delta {N_d}} \over {{N_0} - {N_d}}}} \right)

≈λ+1tΔNdN0−Nd\approx \lambda + {1 \over t}{{\Delta {N_d}} \over {{N_0} - {N_d}}} ,

which gives Δλ=ΔNdt(N0−Nd)\Delta \lambda = {{\Delta {N_d}} \over {t({N_0} - {N_d})}} . Substitute Δ\Delta Nd = 40, t = 1 s, and Nd = 1000 to get Δ\Delta λ\lambda = 0.02.

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