MCQEasyJEE 2023Bohr's Model & Hydrogen Spectrum

JEE Physics 2023 Question with Solution

An electron of a hydrogen-like atom, having Z=4Z = 4, jumps from 4th4^{\text{th}} energy state to 2nd2^{\text{nd}} energy state. The energy released in this process, will be:

(Given Rch=13.6eVRch = 13.6 \, \text{eV})

Where RR = Rydberg constant

cc = Speed of light in vacuum

hh = Planck's constant

  • A

    13.6eV13.6 \, \text{eV}

  • B

    10.5eV10.5 \, \text{eV}

  • C

    3.4eV3.4 \, \text{eV}

  • D

    40.8eV40.8 \, \text{eV}

Answer

Correct answer:A

Step-by-step solution

Standard Method

Given: A hydrogen-like atom with Z=4Z = 4 undergoes a transition from ni=4n_i = 4 to nf=2n_f = 2.

Find: The energy released during the transition and the correct option.

For a hydrogen-like atom, the energy of the electron in the nthn^{\text{th}} orbit is

En=13.6Z2n2eVE_n = -13.6 \frac{Z^2}{n^2} \, \text{eV}

So, the emitted energy is

ΔE=EniEnf=13.6Z2(1nf21ni2)eV\Delta E = E_{n_i} - E_{n_f} = 13.6 Z^2 \left( \frac{1}{n_f^2} - \frac{1}{n_i^2} \right) \, \text{eV}

Substituting Z=4Z = 4, ni=4n_i = 4, and nf=2n_f = 2,

ΔE=13.6×(42)(122142)eV\Delta E = 13.6 \times (4^2) \left( \frac{1}{2^2} - \frac{1}{4^2} \right) \, \text{eV} ΔE=13.6×16(14116)eV\Delta E = 13.6 \times 16 \left( \frac{1}{4} - \frac{1}{16} \right) \, \text{eV} ΔE=13.6×16(4116)eV\Delta E = 13.6 \times 16 \left( \frac{4 - 1}{16} \right) \, \text{eV} ΔE=13.6×16×316eV\Delta E = 13.6 \times 16 \times \frac{3}{16} \, \text{eV} ΔE=13.6×3=40.8eV\Delta E = 13.6 \times 3 = 40.8 \, \text{eV}

Therefore, the energy released is 40.8eV40.8 \, \text{eV}.

The solution working gives 40.8eV40.8 \, \text{eV}, which matches Option D. The solution labels the option as A and also says Option 1, which is inconsistent with the calculation. Hence, the defensible correct option from the working is D.

Common mistakes

  • Using the hydrogen atom value directly without multiplying by Z2Z^2 is incorrect. For hydrogen-like atoms, energy levels scale as Z2Z^2. Always include the factor Z2=16Z^2 = 16 here.

  • Reversing the order of terms in the energy difference can give a wrong sign. For emitted energy, use 1nf21ni2\frac{1}{n_f^2} - \frac{1}{n_i^2} with nf<nin_f < n_i so that the released energy is positive.

  • Confusing orbit numbers n=4n = 4 and n=2n = 2 with their squares leads to wrong fractions. Use 122=14\frac{1}{2^2} = \frac{1}{4} and 142=116\frac{1}{4^2} = \frac{1}{16}, not 12\frac{1}{2} and 14\frac{1}{4}.

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