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Question: A small particle of mass \( m \) moves in such a way that the potential energy \( U = \dfrac{1}{2}m{...

A small particle of mass mm moves in such a way that the potential energy U=12mω2r2U = \dfrac{1}{2}m{\omega ^2}{r^2} where ω\omega is a constant and rr is the distance of the particle from the origin. Assuming Bohr's model of quantisation of angular momentum and circular orbits. Find the radius of the nth allowed orbit is proportional to
(A) nn
(B) n\sqrt n
(C) n13{n^{\dfrac{1}{3}}}
(D) n2{n^2}

Explanation

Solution

Hint : The answer to this problem can be found by equating the given potential energy of the particle and the kinetic energy of the particle. We have to find the radius of the nth orbit so equate the angular momentum of the particle and Bohr’s angular momentum and get the value equate it with the kinetic energy.

Complete step by step answer
Given, The potential energy of the small particle, U=12mω2r2 1U = \dfrac{1}{2}m{\omega ^2}{r^2}{\text{ }} \to {\text{1}}
Where, U is the potential energy of the small particle
ω\omega is a constant
rr is the distance of the particle from the origin
mm is the mass of the small particle
Then the kinetic energy of the small particle, K.E=12mv2 2K.E = \dfrac{1}{2}m{v^2}{\text{ }} \to {\text{2}}
Where,
K.E is the kinetic energy of the small particle
mm is the mass of the small particle
V is the velocity of the particle with which it moves
There is a hint given in the question itself to use the equations of Bohr's model of quantisation of angular momentum and circular orbits
The angular momentum of a particle in nth orbit is,
L=mvr 3L = mvr{\text{ }} \to 3
L is the angular momentum of a particle
mm is the mass of the small particle
V is the velocity of the particle with which it moves
rr is the distance of the particle from the origin
By Bohr’s first postulate, the angular momentum of the electron
L=nh2π 4L = \dfrac{{nh}}{{2\pi }}{\text{ }} \to 4
L is the angular momentum of a particle
n is the orbit in which it revolves
h is the Planck constant
Equating 3 and 4 we get
mvr=nh2πmvr = \dfrac{{nh}}{{2\pi }}
mv=nh2πr 5mv = \dfrac{{nh}}{{2\pi r}}{\text{ }} \to 5
Substitute equation 5 in equation 2
K.E=12(nh2πr)2K.E = \dfrac{1}{2}{\left( {\dfrac{{nh}}{{2\pi r}}} \right)^2}
K.E=14n2h2π2r2 6K.E = \dfrac{1}{4}\dfrac{{{n^2}{h^2}}}{{{\pi ^2}{r^2}}}{\text{ }} \to {\text{6}}
We know that,
Kinetic energy =12potential energyKinetic{\text{ }}energy{\text{ }} = \dfrac{1}{2}{}potential{\text{ }}energy
Then, from equation 1 and equation 6
14n2h2π2r2=12(12mω2r2)\dfrac{1}{4}\dfrac{{{n^2}{h^2}}}{{{\pi ^2}{r^2}}} = \dfrac{1}{2}\left( {\dfrac{1}{2}m{\omega ^2}{r^2}} \right)
n2h2π2r2=mω2r2\dfrac{{{n^2}{h^2}}}{{{\pi ^2}{r^2}}} = m{\omega ^2}{r^2}
n2h2π2r2mω2=r2\dfrac{{{n^2}{h^2}}}{{{\pi ^2}{r^2}m{\omega ^2}}} = {r^2}
n2h2π2mω2=r2×r2\dfrac{{{n^2}{h^2}}}{{{\pi ^2}m{\omega ^2}}} = {r^2} \times {r^2}
r4=n2h2π2mω2{r^4} = \dfrac{{{n^2}{h^2}}}{{{\pi ^2}m{\omega ^2}}}
From above equation we get
r4n2{r^4} \propto {n^2}
rnr \propto \sqrt n
The radius, rr of orbit is proportional to n\sqrt n (square root of n)
Hence the correct answer is option (B) n\sqrt n .

Note
It is an indirect question since we have to find the relation between the radius and the nth orbit, we are using the equations having n (nth orbit) and r (radius) to relate them. It is given in the question to Assume Bohr's model of quantisation of angular momentum and circular orbits.