Question

Two independent harmonic oscillators of equal mass are oscillating about the origin with angular frequencies ${\omega }_1$ and ${\omega }_2$ and have total energies $E_1$ and $E_2$​, respectively. The variations of their momenta p with positions x are shown in figures. If ${\displaystyle \frac{a}{b}}=n^2$ and ${\displaystyle \frac{a}{R}}=n$, then the correct equation(s) is (are)

$\begin{array}{rl}& \text{A}\text{. }{E}_1{\omega }_1=E_2{\omega }_2\\ & \text{B}\text{. }{\displaystyle \frac{{\omega }_2}{{\omega }_1}}=n^2\\ & \text{C}\text{. }{\omega }_1{\omega }_2=n^2\\ & \text{D}\text{. }{\displaystyle \frac{E_1}{{\omega }_1}}={\displaystyle \frac{E_2}{{\omega }_2}}\end{array}$

Answer 1

Hint: We have two different particles undergoing independent harmonic oscillations and the mass of them are the same. We are given the angular frequencies and energies of the two systems. From the given figure we can identify their path and find the maximum momenta and their energies, then by using the given relations we will get the correct expressions.

Formula used:
$p=mv$
$E={\displaystyle \frac{1}{2}}m{\omega }^2{a}^2$

Complete step-by-step answer:
In the question we are given two independent harmonic oscillations with equal mass.
The angular frequencies of the two oscillations are ${\omega }_1$ and ${\omega }_2$ and their energies are $E_1$ and $E_2$ respectively.
Let us consider the first case.

From the figure we can see that the particle in this oscillation has an elliptical path.
We know that the momentum is given by the equation,
$p=mv$, were ‘m’ is the mass and ‘v’ is the velocity.
Therefore the maximum momentum will be,
$p_{max}=m{v}_{max}$
Since the maximum velocity, $v_{max}=r\omega$, were ‘r’ is the radius and ‘$\omega$’ is the angular frequency, we get the maximum momentum as,
$p_{max}=mr\omega$
Therefore in the first case, since it is an elliptical path the radius is taken as ‘a’ and from the figure we can see that ‘b’ is the maximum momentum.
Therefore we get,
$\Rightarrow p_{max}=b=ma{\omega }_1$
Now let us consider case 2.

From the figure we can see that the particle in this oscillation has a circular path.
We know that the maximum momentum is,
$p_{max}=mr\omega$
In this case, from the figure we can see that the radius and the maximum momentum is ‘R’. therefore we get,
$\Rightarrow p_{max}=R=mR{\omega }_2$
$\Rightarrow m{\omega }_2=1$
Thus we have the maximum momentum in case 1 and 2 as $b=ma{\omega }_1$ and $m{\omega }_2=1$ respectively.
By dividing these two equations we get,
$\Rightarrow {\displaystyle \frac{b}{1}}={\displaystyle \frac{ma{\omega }_1}{m{\omega }_2}}$
Since the mass is equal in both the cases. We can eliminate the mass.
$\Rightarrow {\displaystyle \frac{b}{a}}={\displaystyle \frac{{\omega }_1}{{\omega }_2}}$
In the question it is given that ${\displaystyle \frac{a}{b}}=n^2$
Therefore we know that, ${\displaystyle \frac{b}{a}}={\displaystyle \frac{1}{n^2}}$
By substituting this we will get,
$\Rightarrow {\displaystyle \frac{{\omega }_1}{{\omega }_2}}={\displaystyle \frac{b}{a}}={\displaystyle \frac{1}{n^2}}$
$\Rightarrow {\displaystyle \frac{{\omega }_1}{{\omega }_2}}={\displaystyle \frac{1}{n^2}}$
Therefore we get,
$\Rightarrow {\displaystyle \frac{{\omega }_2}{{\omega }_1}}=n^2$
Hence option B is correct.
Now let us consider the energy in both the cases.
In the first case, we will get the energy as,
$E_1=m{{\omega }_1}^2{a}^2$
$E_2=m{{\omega }_2}^2{R}^2$
By dividing these two equations, we will get
$\Rightarrow {\displaystyle \frac{E_1}{E_2}}={\displaystyle \frac{m{{\omega }_1}^2{a}^2}{m{{\omega }_2}^2{R}^2}}$
$\Rightarrow {\displaystyle \frac{E_1}{E_2}}={\displaystyle \frac{{{\omega }_1}^2{a}^2}{{{\omega }_2}^2{R}^2}}$
From the question we know that, ${\displaystyle \frac{a}{R}}=n$
Therefore we know that $\Rightarrow {\displaystyle \frac{a^2}{R^2}}=n^2$
Thus the ratio of the energies will become,
$\Rightarrow {\displaystyle \frac{E_1}{E_2}}={\displaystyle \frac{{{\omega }_1}^2}{{{\omega }_2}^2}}\times n^2$
From previous calculation we know that,
$n^2={\displaystyle \frac{{\omega }_2}{{\omega }_1}}$
By substituting this in the ratio equation, we will get
$$\Rightarrow {\displaystyle \frac{E_1}{E_2}}={\displaystyle \frac{{{\omega }_1}^2}{{{\omega }_2}^2}}\times {\displaystyle \frac{{\omega }_2}{{\omega }_1}}$$
$$\Rightarrow {\displaystyle \frac{E_1}{E_2}}={\displaystyle \frac{{\omega }_1}{{\omega }_2}}$$
$$\Rightarrow {\displaystyle \frac{E_1}{{\omega }_1}}={\displaystyle \frac{E_2}{{\omega }_2}}$$
Therefore option D is also correct.

So, the correct answer is “Option B and D”.

Note: A periodic oscillation is an oscillation when the periodic motion repeats at fixed intervals. Simple harmonic motion or SHM is a special type of periodic oscillation. In simple harmonic motion the restoring force of the moving object will be always directly proportional to the magnitude of displacement of the object and its direction will be toward the mean position.