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Question: Two particles of masses \[{m_1}\] and \({m_2}\) are connected by a rigid massless rod of length \(r\...

Two particles of masses m1{m_1} and m2{m_2} are connected by a rigid massless rod of length rr to constitute a dumbbell. The moment of inertia of the dumbbell about an axis perpendicular to the rod and passing through the center of mass is:
A. m1m2r2m1+m2\dfrac{{{m_1}{m_2}{r^2}}}{{{m_1} + {m_2}}}
B. (m1+m2)r2\left( {{m_1} + {m_2}} \right){r^2}
C. m1m2r2m1m2\dfrac{{{m_1}{m_2}{r^2}}}{{{m_1} - {m_2}}}
D. (m1m2)r2\left( {{m_1} - {m_2}} \right){r^2}

Explanation

Solution

We will first calculate the center of mass of the dumbbell from masses m1{m_1} and m2{m_2}. Then we will calculate the moment of inertia of both the masses m1{m_1} and m2{m_2} about the center of mass of both the masses. Now, the moment of inertia of the dumbbell about an axis perpendicular to the rod and passing through the center of mass can be calculated by adding the center of mass of masses m1{m_1} and m2{m_2}.

Complete step by step answer:
In this question, there are two masses m1{m_1} and m2{m_2} that are connected by a rigid massless rod of length rr.
The position of center of mass of the dumbbell from mass m1{m_1} is given below
M1=m2rm1+m2{M_1} = \dfrac{{{m_2}r}}{{{m_1} + {m_2}}}
Also, the position of center of mass of the dumbbell from mass m2{m_2} is given below
M2=m1rm1+m2{M_2} = \dfrac{{{m_1}r}}{{{m_1} + {m_2}}}
Now, the moment of inertia of the mass m1{m_1} about the center of mass of the dumbbell from mass m1{m_1} is given below
I1=m1×(m2rm1+m2)2{I_1} = {m_1} \times {\left( {\dfrac{{{m_2}r}}{{{m_1} + {m_2}}}} \right)^2}
I1=m1m22r2(m1+m2)2\Rightarrow \,{I_1} = \dfrac{{{m_1}m_2^2{r^2}}}{{{{\left( {{m_1} + {m_2}} \right)}^2}}}
Also, the moment of inertia of mass m2{m_2} about the center of mass of the dumbbell from mass m2{m_2} is given below
I2=m2×(m1rm1+m2)2{I_2} = {m_2} \times {\left( {\dfrac{{{m_1}r}}{{{m_1} + {m_2}}}} \right)^2}
I2=m2m12r2(m1+m2)2\Rightarrow \,{I_2} = \dfrac{{{m_2}m_1^2{r^2}}}{{{{\left( {{m_1} + {m_2}} \right)}^2}}}
Now, the moment of inertia of the dumbbell about an axis perpendicular to the rod and passing through the center of mass can be calculated by adding the center of mass of masses m1{m_1} and m2{m_2} as given below
I=I1+I2I = {I_1} + {I_2}
I=m1m22r2(m1+m2)2+m2m12r2(m1+m2)2\Rightarrow \,I = \dfrac{{{m_1}m_2^2{r^2}}}{{{{\left( {{m_1} + {m_2}} \right)}^2}}} + \dfrac{{{m_2}m_1^2{r^2}}}{{{{\left( {{m_1} + {m_2}} \right)}^2}}}
I=m1m2(m1+m2)r2(m1+m2)2\Rightarrow \,I = \dfrac{{{m_1}{m_2}\left( {{m_1} + {m_2}} \right){r^2}}}{{{{\left( {{m_1} + {m_2}} \right)}^2}}}
I=m1m2r2m1+m2\therefore\,I = \dfrac{{{m_1}{m_2}{r^2}}}{{{m_1} + {m_2}}}
Therefore, the moment of inertia of the dumbbell about an axis perpendicular to the rod and passing through the center of mass is m1m2r2m1+m2\dfrac{{{m_1}{m_2}{r^2}}}{{{m_1} + {m_2}}}.

Hence, option A is the correct option.

Note: Here remember that the center of mass of mass m1{m_1} will be in terms of m2{m_2}. On the other hand, the center of mass of m2{m_2} will be in terms of m1{m_1}. Also, the moment of inertia of mass m1{m_1} will be the product of mass and the center of mass of m1{m_1}. On the other hand, the moment of inertia of mass m2{m_2} will be the product of mass and the center of mass of m2{m_2}.