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Question: A diatomic molecule is formed by two atoms which may be treated as mass points \(m_1\) and \(m_2\) j...

A diatomic molecule is formed by two atoms which may be treated as mass points m1m_1 and m2m_2 joined by a massless rod of length r. Then, the moment of inertia of the molecule about an axis passing through the center of mass and perpendicular to rod is:
A. Zero
B. (m1+m2)r2({m_1} + m{}_2){r^2}
C. (m1+m2m1m2)r2(\dfrac{{{m_1} + {m_2}}}{{{m_1}{m_2}}}){r^2}
D. (m1m2m1+m2)r2(\dfrac{{{m^{_{}}}_1{m_2}}}{{{m_1} + {m_2}}}){r^2}

Explanation

Solution

Hint: for this we need to have basic knowledge of center of mass and moment of inertia. Moment of Inertia can be defined as how easily a body can be rotated about a given axis. It is a rotational analogue of mass.

Step by step solution:

1. Let us first draw a figure which will help us in better understanding of the Question.
Below we have drawn a rod AB where m1m_1 is the mass at point A and m2m_2 is the mass at point B. At point O we have assumed the center of mass of the rod. We have drawn a perpendicular axis to the rod about which moment of inertia is to be calculated. Let r1r_1 be the distance between point A and O and r2r_2 be the distance between point B and O.

2. As we know that the position of center of mass of the particles is given by
X=m1x1+m2x2+.......mnxnm1+m2+.....mn=miximiX = \dfrac{{{m_1}{x_1} + {m_2}{x_2} + .......{m_n}{x_n}}}{{{m_1} + {m_2} + .....{m_n}}} = \dfrac{{\sum {{m_i}{x_i}} }}{{\sum {{m_i}} }} …………….equation 1
So here according to our figure we have r1=m1×0+m2×rm1+m2{r_1} = \dfrac{{{m_1} \times 0 + {m_2} \times r}}{{{m_1} + {m_2}}} because m1m_1 is at the 0 distance from point A and m2m_2 is at the distance r from point A.
Again r1=m2×rm1+m2{r_1} = \dfrac{{{m_2} \times r}}{{{m_1} + {m_2}}} ………………equation 2
And r2=rm2×rm1+m2{r_2} = r - \dfrac{{{m_2} \times r}}{{{m_1} + {m_2}}} ……………..equation 3

3. Now Moment of Inertia is given by I=m1x12+m2x22+.........mnxn2I = {m_1}{x_1}^2 + {m_2}{x_2}^2 + .........{m_n}{x_n}^2
Here in our question I=m1r12+m2r22I = {m_1}{r_1}^2 + {m_2}{r_2}^2
With the help of equations 2 and 3 we get
I=m1m22r2(m1+m2)2+m12m2r2(m1+m2)2I = \dfrac{{{m_1}{m_2}^2{r^2}}}{{{{({m_1} + {m_2})}^2}}} + \dfrac{{{m_1}^2{m_2}{r^2}}}{{{{({m_1} + {m_2})}^2}}}
Now taking some common terms
I=m1m2r2(m1+m2)2(m1+m2)I = \dfrac{{{m_1}{m_2}{r^2}}}{{{{({m_1} + {m_2})}^2}}}({m_1} + {m_2})
After doing the simplifications we get:
I=m1m2r2m1+m2I = \dfrac{{{m_1}{m_2}{r^2}}}{{{m_1} + {m_2}}}
Or it can also be written as I=(m1m2m1+m2)r2I = (\dfrac{{{m_1}{m_2}}}{{{m_1} + {m_2}}}){r^2}
Hence option D is correct.

Note: In this question basic knowledge of moment of inertia and simple algebra is used. We can also solve this type of question using numerical values instead of variables.