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QJEEAdv19Phe381: JEE Advanced 2019 Physics - Class 12 JEEAdv19Phe381 Solution: A free hydrogen atom after absorbing a photon of wavelength a…

A free hydrogen atom after absorbing a photon of wavelength λ\lambda a gets excited from the state n = 1 to the state n = 4. Immediately after that the electron jumps to n = m state by emitting a photon of wavelength λ\lambda e. Let the change in momentum of atom due to the absorption and the emission be Δpa\Delta {p_a} and Δpe\Delta {p_e} , respectively. If λaλe=15{{{\lambda _a}} \over {{\lambda _e}}} = {1 \over 5} , which of the option(s) is/are correct? [Use hc = 1242 eVnm; 1 nm = 10-9 m, h and c are Planck's constant and speed of light in vacuum, respectively]

Multiple Choice Options

  • A The ratio of kinetic energy of the electron in the state n = m to the state, n = 1 is 14{1 \over 4}
  • B m = 2
  • C ΔpaΔpe=12{{\Delta {p_a}} \over {\Delta {p_e}}} = {1 \over 2}
  • D λ\lambda e = 418 nm

Step-by-Step Verified Solution

A hydrogen atom in its ground state (n = 1) absorbs a photon with wavelength λa\lambda_a and gets excited to the n = 4 state. Subsequently, the electron transitions to the n = m state, emitting a photon with wavelength λe\lambda_e . Given that λaλe=15{{{\lambda _a}} \over {{\lambda _e}}} = {1 \over 5} , let's analyze the options systematically.

Calculation for the Wavelengths:

The energy difference between levels in a hydrogen atom can be given by the Rydberg formula for hydrogen:

En=−13.6 eVn2E_n = - \frac{{13.6 \ eV}}{{n^2}}

The energy of the absorbed photon that excites the electron from n = 1 to n = 4 could be expressed as:

Ea=E4−E1=−13.6 eV42−(−13.6 eV12)=−13.6 eV16+13.6 eV=13.6 eV(1−116)=13.6 eV⋅1516=12.75 eVE_a = E_4 - E_1 = - \frac{{13.6 \ eV}}{{4^2}} - (- \frac{{13.6 \ eV}}{{1^2}}) = - \frac{{13.6 \ eV}}{{16}} + 13.6 \ eV = 13.6 \ eV (1 - \frac{1}{16}) = 13.6 \ eV \cdot \frac{15}{16} = 12.75 \ eV

Wavelength λa\lambda_a associated with this energy is:

λa=hcEa=1242 nm⋅eV12.75 eV=97.4 nm\lambda_a = \frac{{hc}}{{E_a}} = \frac{{1242 \ nm \cdot eV}}{{12.75 \ eV}} = 97.4 \ nm

Given λaλe=15{{{\lambda _a}} \over {{\lambda _e}}} = {1 \over 5} , we get:

λe=5λa=5⋅97.4 nm=487 nm\lambda_e = 5 \lambda_a = 5 \cdot 97.4 \ nm = 487 \ nm

Option A: The ratio of kinetic energy of the electron in the state n = m to the state n = 1 is 14{1 \over 4}

The kinetic energy of an electron in a hydrogen atom in the nth state is proportional to −1n2- \frac{{1}}{{n^2}} . Therefore, the ratio of kinetic energy in state m to that in state n can be written as:

EmE1=−13.6m2eV−13.6 eV=1m2\frac{{E_m}}{{E_1}} = \frac{{- \frac{{13.6}}{{m^2}} eV}}{{- 13.6 \ eV}} = \frac{1}{{m^2}}

According to the question, the ratio is 14\frac{1}{4} :

1m2=14⇒m=2\frac{1}{{m^2}} = \frac{1}{4} \Rightarrow m = 2

Therefore, Option A is correct if m = 2.

Option B: m = 2

Based on the energy calculations above, we find m = 2. Therefore, Option B is correct.

Option C: ΔpaΔpe=12{{\Delta {p_a}} \over {\Delta {p_e}}} = {1 \over 2}

The change in momentum for each photon is given by:

Δp=hλ\Delta p = \frac{h}{\lambda}

So, the ratio of the momentum changes is:

ΔpaΔpe=hλahλe=λeλa=5\frac{{\Delta p_a}}{{\Delta p_e}} = \frac{{\frac{h}{\lambda_a}}}{{\frac{h}{\lambda_e}}} = \frac{\lambda_e}{\lambda_a} = 5

This shows the given option C (i.e., 12\frac{1}{2} ) is incorrect. The correct ratio is 5.

Option D: λe=418 nm\lambda_e = 418 \ nm

From our previous calculations, we found λe=487 nm\lambda_e = 487 \ nm , which does not match 418 nm. Option D is incorrect.

Hence, the correct options are A and B.

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