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QJEEAdv21Ph9ee7: JEE Advanced 2021 Physics - Class 12 JEEAdv21Ph9ee7 Solution: Which of the following statement(s) is(are) correct about the…

Which of the following statement(s) is(are) correct about the spectrum of the hydrogen atom?

Multiple Choice Options

  • A The ratio of the longest wavelength to the shortest wavelength in Balmer series is 9/5
  • B There is an overlap between the wavelength ranges of Balmer and Paschen series
  • C The wavelengths of Lyman series are given by (1+1m2)λ0\left( {1 + {1 \over {{m^2}}}} \right){\lambda _0} , where λ0{\lambda _0} is the shortest wavelength of Lyman series and m is an integer
  • D The wavelength ranges of Lyman and Balmer series do not overlap

Step-by-Step Verified Solution

For Balmer series

\frac{1}{\lambda}=\mathrm{R}\left(\frac{1}{4}-\frac{1}{n^2}\right) n>2

λ\lambda is minimum for transition from n1→∞n_1 \rightarrow \infty to n2=2n_2=2 .

1λmin⁡=R4\frac{1}{\lambda_{\min }}=\frac{R}{4}

λ\lambda is maximum for transition from n1=3n_1=3 to n2=2n_2=2

1λmax⁡=R(14−19)=5R36\frac{1}{\lambda_{\max }}=\mathrm{R}\left(\frac{1}{4}-\frac{1}{9}\right)=\frac{5 \mathrm{R}}{36}

Dividing the above two equations, we get

λmax⁡λmin⁡=R4×365R=95\frac{\lambda_{\max }}{\lambda_{\min }}=\frac{R}{4} \times \frac{36}{5 R}=\frac{9}{5}

Option (A) is correct.

For Lyman series,

λmin⁡=91.18 nm\lambda_{\min }=91.18 \mathrm{~nm}

λmax⁡=121.57 nm\lambda_{\max }=121.57 \mathrm{~nm}

For Balmer series,

λmin⁡=364.60 nm\lambda_{\min }=364.60 \mathrm{~nm}

λmax⁡=656.30 nm\lambda_{\max }=656.30 \mathrm{~nm}

For Pashen series,

λmin⁡=820.40 nm\lambda_{\min }=820.40 \mathrm{~nm}

λmax⁡=1875 nm\lambda_{\max }=1875 \mathrm{~nm}

We can see from the above that there is no overlap between the wavelength ranges of Balmer and Paschen series. so, option (B) is incorrect.

Similarly wavelength ranges of Lyman and Balmer series also do not overlap. Hence, option (D) is correct.

Shortest wavelength of Lyman series

1λ0amp;=R(1−1∞)λ0amp;=1R\begin{aligned}\frac{1}{\lambda_0} & =R\left(1-\frac{1}{\infty}\right) \\\\\lambda_0 & =\frac{1}{R}\end{aligned}

For Lyman series, 1λ=R(1−1n2)\frac{1}{\lambda}=\mathrm{R}\left(1-\frac{1}{n^2}\right)

amp;=1λ0(1−1n2)λamp;=λ01−1n2=λ0n2n2−1amp;=λ0(n2−1)+1n2−1amp;=λ0(1+1n2−1)\begin{aligned}& =\frac{1}{\lambda_0}\left(1-\frac{1}{n^2}\right) \\\\\lambda & =\frac{\lambda_0}{1-\frac{1}{n^2}}=\frac{\lambda_0 n^2}{n^2-1} \\\\& =\frac{\lambda_0\left(n^2-1\right)+1}{n^2-1} \\\\& =\lambda_0\left(1+\frac{1}{n^2-1}\right)\end{aligned}

If n2−1=m2n^2-1=m^2 ( mm is an integer)

then this is rarely true as (n2−1)\left(n^2-1\right) cannot always be the square of an integer. Hence, option (C) is incorrect.

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