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The wavelength of radiation emitted is ' $\lambda_0$ ' when an electron jumps from the second excited state to the first excited state of hydrogen atom. If the electron jumps from the third excited state to the second orbit of the hydrogen atom, the wavelength of the radiation emitted will be $\frac{20}{x} \lambda_0$. The value of $x$ is
PhysicsDual Nature of MatterMHT CETMHT CET 2023 (12 May Shift 1)
Options:
  • A $3$
  • B $9$
  • C $13$
  • D $27$
Solution:
2030 Upvotes Verified Answer
The correct answer is: $27$
According to Rydberg's formula, $\frac{1}{\lambda}=\mathrm{R}\left(\frac{1}{\mathrm{n}_1^2}-\frac{1}{\mathrm{n}_2^2}\right)$
When electron jumps from $2^{\text {nd }}$ exited state to first exited state, $\mathrm{n}_2=3, \mathrm{n}_1=2, \lambda=\lambda_0$, we get
$$
\frac{1}{\lambda_0}=\mathrm{R}\left(\frac{1}{2^2}-\frac{1}{3^2}\right)
$$
When electron jumps from $3^{\text {rd }}$ exited state to $2^{\text {nd }}$ orbit,
$\mathrm{n}_2=4, \mathrm{n}_1=2$, we get
$$
\frac{1}{\lambda}=\mathrm{R}\left(\frac{1}{4^2}-\frac{1}{2^2}\right)
$$
$$
\begin{aligned}
\therefore \quad \frac{\lambda}{\lambda_0} & =\frac{\mathrm{R}\left(\frac{1}{2^2}-\frac{1}{3^2}\right)}{\mathrm{R}\left(\frac{1}{2^2}-\frac{1}{4^2}\right)} \\
& =\frac{5}{36} \times \frac{16}{3}=\frac{20}{27}
\end{aligned}
$$
$$
\begin{aligned}
& \therefore \quad \lambda=\frac{20}{27} \lambda_0 \\
& \Rightarrow \mathrm{x}=27
\end{aligned}
$$

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