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Question: The radius of the orbit of an electron in a Hydrogen-like atom is \( 4.5{{a}_{0}} \) where \( {{a}_{...

The radius of the orbit of an electron in a Hydrogen-like atom is 4.5a04.5{{a}_{0}} where a0{{a}_{0}} the Bohr radius is. Its orbital angular momentum is 3h2π\dfrac{3h}{2\pi } . It is given that hh is Planck's constant and RR is Rydberg constant. The possible wavelength(s), if the atom excited will be,
There may be multiple correct answers for this question.
A.932R B.916R C.95R D.43R \begin{aligned} & A.\dfrac{9}{32R} \\\ & B.\dfrac{9}{16R} \\\ & C.\dfrac{9}{5R} \\\ & D.\dfrac{4}{3R} \\\ \end{aligned}

Explanation

Solution

First of all find the nn and ZZ value using the equation for the radius of the orbit the possible wavelength can be determined by the equation,
r=a0n2Zr={{a}_{0}}\dfrac{{{n}^{2}}}{Z}
Then find out the possible wavelength using the equation,
1λ=RZ2[1n121n22]\dfrac{1}{\lambda }=R{{Z}^{2}}\left[ \dfrac{1}{{{n}_{1}}^{2}}-\dfrac{1}{{{n}_{2}}^{2}} \right]
Where RR be the Rydberg constant, n1{{n}_{1}} and n2{{n}_{2}} be the level of orbital or the position of orbital and ZZ be the atomic number. Chances are there for multiple correct answers.

Complete step-by-step answer:
It is already given that, the radius of orbit of an electron in a Bohr orbit is,
r=4.5a0r=4.5{{a}_{0}}
The radius of the Bohr orbit is generally given as,
r=a0n2Zr={{a}_{0}}\dfrac{{{n}^{2}}}{Z}
Therefore we can equate both these equations together,
a0n2Z=4.5a0{{a}_{0}}\dfrac{{{n}^{2}}}{Z}=4.5{{a}_{0}}
And also we can write that,
nh2π=3h2π\dfrac{nh}{2\pi }=\dfrac{3h}{2\pi }
So from this we can write that,
n=3n=3 and Z=2Z=2
Therefore now we can find the possible wavelength which is given by the equation,
1λ=RZ2[1n121n22]\dfrac{1}{\lambda }=R{{Z}^{2}}\left[ \dfrac{1}{{{n}_{1}}^{2}}-\dfrac{1}{{{n}_{2}}^{2}} \right]
Here three types of transition are possible, one can be from first state to third state.
This can be found using the above mentioned equation.
Substituting the values in it,

& \dfrac{1}{{{\lambda }_{1}}}=R{{Z}^{2}}\left[ \dfrac{1}{{{1}^{2}}}-\dfrac{1}{{{3}^{2}}} \right] \\\ & {{\lambda }_{1}}=\dfrac{9}{32R} \\\ \end{aligned}$$ Another possibility is that the transition can take place from second state to the first one, $$\begin{aligned} & \dfrac{1}{{{\lambda }_{2}}}=R{{Z}^{2}}\left[ \dfrac{1}{{{1}^{2}}}-\dfrac{1}{{{2}^{2}}} \right] \\\ & {{\lambda }_{2}}=\dfrac{1}{3R} \\\ \end{aligned}$$ And the last possibility is that, the transition may happens from second state to the third state, $$\begin{aligned} & \dfrac{1}{{{\lambda }_{3}}}=R{{Z}^{2}}\left[ \dfrac{1}{{{2}^{2}}}-\dfrac{1}{{{3}^{2}}} \right] \\\ & {{\lambda }_{3}}=\dfrac{9}{5R} \\\ \end{aligned}$$ In the given options, there are two options which are having these found out values in it. **So, the correct answers are “Option A and C”.** **Note:** In physics, the Rydberg constant is defined as a physical constant which is in relation with atomic spectra. It is abbreviated as $ R $. Rydberg constant was firstly found from the Rydberg formula as a mere constant. Later Niels Bohr developed it from the fundamental constants.