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MHT CET 202624 AprilEvening Shift
Exam
MHT CET
Year
2026
Date
24 April
Shift
Evening Shift
Subject
Physics
Chapter
Atomic Physics

MHT CET 2026 · 24 April · Evening Shift · Physics · Atomic Physics

The radius of the orbit of an electron in a hydrogen like atom is...

The radius of the orbit of an electron in a hydrogen like atom is 4.5a04.5a_0, where a0a_0 is the Bohr radius. Its orbital angular momentum is 3h2π\dfrac{3h}{2\pi}. It is given than h is Planck's constant and R is Rydberg's constant. The possible wavelength (λ)(\lambda), when the transition of atom from higher energy level to lower energy level, is

Options

  1. A932R\dfrac{9}{32R}
  2. B916R\dfrac{9}{16R}
  3. C910R\dfrac{9}{10R}
  4. D43R\dfrac{4}{3R}

Correct answer

A. 932R\dfrac{9}{32R}

Step-by-step solution

The orbital angular momentum of an electron is given by L=nh2πL = \dfrac{nh}{2\pi}.

Given L=3h2πL = \dfrac{3h}{2\pi}, we get n=3n = 3.

The radius of the nn-th orbit in a hydrogen-like atom is r=n2Za0r = \dfrac{n^2}{Z}a_0.

Substituting r=4.5a0andn=3r = 4.5a_0 and n = 3:

4.5a0=32Za0⇒Z=94.5=24.5a_0 = \dfrac{3^2}{Z}a_0 \Rightarrow Z = \dfrac{9}{4.5} = 2

The possible transitions from the n=3n = 3 state to lower energy levels are n=3→1andn=3→2n = 3 \rightarrow 1 and n = 3 \rightarrow 2.

Using the Rydberg formula for wavelength:

1λ=RZ2(1nf2−1ni2)<br><br>Forthetransition\dfrac{1}{\lambda} = RZ^2 \left( \dfrac{1}{n_f^2} - \dfrac{1}{n_i^2} \right)<br><br>For the transition n = 3 → 1:<br><br>1λ=:<br><br>\dfrac{1}{\lambda} = R(2)^2 \left( \dfrac{1}{1^2} - \dfrac{1}{3^2} \right) =4R \left(1 - \dfrac{1}{9} \right) =4R \left( \dfrac{8}{9} \right) = \dfrac{32R}{9}

λ=\lambda =\dfrac{9}{32R}

Forthetransitionn=3→2the transition n = 3 → 2:

\dfrac{1}{\lambda} =R(2)2(122−132)=4R(14−19)=4R(536)=5R9<br><br>R(2)^2 \left( \dfrac{1}{2^2} - \dfrac{1}{3^2} \right) =4R \left( \dfrac{1}{4} - \dfrac{1}{9} \right) =4R \left( \dfrac{5}{36} \right) = \dfrac{5R}{9}<br><br>\lambda = 95R<br><br>Among\dfrac{9}{5R}<br><br>Among the given options,932R\dfrac{9}{32R} is a possible wavelength.

Answer: 932R\dfrac{9}{32R}
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