MCQEasyJEE 2025Bohr's Model & Hydrogen Spectrum

JEE Physics 2025 Question with Solution

For a hydrogen atom, the ratio of the largest wavelength of the Lyman series to that of the Balmer series is:

  • A

    5:365 : 36

  • B

    5:275 : 27

  • C

    3:43 : 4

  • D

    27:527 : 5

Answer

Correct answer:B

Step-by-step solution

Standard Method

Given: A hydrogen atom is considered, and we need the ratio of the largest wavelength of the Lyman series to that of the Balmer series.

Find: λLymanλBalmer\dfrac{\lambda_{\text{Lyman}}}{\lambda_{\text{Balmer}}}

Use the Rydberg formula:

1λ=RH(1n121n22)\frac{1}{\lambda} = R_H \left( \frac{1}{n_1^2} - \frac{1}{n_2^2} \right)

For the Lyman series, transitions end at n1=1n_1 = 1. For the Balmer series, transitions end at n1=2n_1 = 2.

The largest wavelength in a series corresponds to the smallest energy gap, so we take the first line of each series.

For the Lyman series, the largest wavelength corresponds to the transition n2=2n1=1n_2 = 2 \to n_1 = 1:

1λLyman=RH(112122)=RH(114)=3RH4\frac{1}{\lambda_{\text{Lyman}}} = R_H \left( \frac{1}{1^2} - \frac{1}{2^2} \right) = R_H \left( 1 - \frac{1}{4} \right) = \frac{3R_H}{4}

Therefore,

λLyman=43RH\lambda_{\text{Lyman}} = \frac{4}{3R_H}

For the Balmer series, the largest wavelength corresponds to the transition n2=3n1=2n_2 = 3 \to n_1 = 2:

1λBalmer=RH(122132)=RH(1419)=5RH36\frac{1}{\lambda_{\text{Balmer}}} = R_H \left( \frac{1}{2^2} - \frac{1}{3^2} \right) = R_H \left( \frac{1}{4} - \frac{1}{9} \right) = \frac{5R_H}{36}

Therefore,

λBalmer=365RH\lambda_{\text{Balmer}} = \frac{36}{5R_H}

Now take the ratio:

λLymanλBalmer=43RH365RH=43×536=527\frac{\lambda_{\text{Lyman}}}{\lambda_{\text{Balmer}}} = \frac{\frac{4}{3R_H}}{\frac{36}{5R_H}} = \frac{4}{3} \times \frac{5}{36} = \frac{5}{27}

Therefore, the correct option is B.

Common mistakes

  • Taking the series limit instead of the largest wavelength is incorrect. The largest wavelength comes from the smallest energy gap, which is the first transition of the series: 212 \to 1 for Lyman and 323 \to 2 for Balmer.

  • Using the ratio of 1λ\dfrac{1}{\lambda} values directly as the ratio of wavelengths is wrong. Since wavelength is the reciprocal quantity here, you must invert after applying the Rydberg formula.

  • Confusing the lower levels of the series gives a wrong setup. Lyman ends at n1=1n_1 = 1, while Balmer ends at n1=2n_1 = 2. Always identify the correct final energy level before substitution.

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