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Motion of the centre of mass is considered one the most difficult concept.
18 Questions around this concept.
Two identical particles move towards each other with velocity and
respectively. The velocity of the centre of mass is :
A body of mass M while falling vertically downwards under gravity breaks into two parts; a body B of mass
and another body
of mass
. The center of mass of bodies B and
taken together shifts compared to that of the body
towards :
Two particles of masses $m_1$ and $m_2\left(m_1>m_2\right)$ have only mutual interaction force between them. If particles are released from rest then the velocity of the centre of mass will be
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Two particles of mass 2kg and 3kg one moving as shown in the figure. The velocity of the center of mass of the system will be
Two particles A and B, initially at rest, move towards each other under a mutual force of attraction. At the instant when the speed of A is u and the speed of B is 2 u, the speed of centre of mass is
Velocity of the centre of mass
$
\vec{v}_{C M}=\frac{m_1 \overrightarrow{v_1}+m_2 \vec{v}_2 \ldots \ldots \ldots}{m_1+m_2 \ldots \ldots}
$
$\mathrm{m}_1, \mathrm{~m}_2----$ are mass of all the particles $\overrightarrow{v_1}, \vec{v}_2 \ldots \ldots$ are velocities of all the particles.
Similarly momentum of the system $=P_{\text {sys }}=M v_{c m}$
Acceleration of centre of mass
$
\vec{a}_{C M}=\frac{m_1 \overrightarrow{a_1}+m_2 \vec{a}_2 \ldots \ldots \ldots}{m_1+m_2 \ldots \ldots}
$
$\mathrm{m}_1, \mathrm{~m}_2$ are mass of all the particles $\overrightarrow{a_1}, \overrightarrow{a_2} \cdots$ are their respective acceleration.
Similarly Net force on the system $=F_{\text {net }}=M a_{c m}$
And $F_{n e t}=\overrightarrow{F_{e x t}}+\overrightarrow{F_{\text {int }}}$
And we know that both the action and reaction of an internal force must be within the system. In this way, vector summation will cancel all internal forces and hence net internal force on the system is zero.
So $\overrightarrow{F_{\text {net }}}=M \overrightarrow{a_{c m}}$
If External Force = 0
$
\vec{F}_{e x t}=0 \Rightarrow M \vec{a}_{c m}=0 \Rightarrow \vec{a}_{c m}=0
$
if $\vec{a}_{c m}=0 \Rightarrow v_{c m}=$ constant
${ }_{\text {If }} v_{c m}=$ constant $\Rightarrow P_{\text {sys }}=$ constant
So it implies that the total momentum of the system must remain constant.
i.e. if no external force is acting on the system, the net momentum of the system remains constant. This is nothing but the principle of conservation of momentum in absence of external forces. Which says ìf resultant external force is zero on the system, then the net momentum of the system must remain constant.
Special case
If External Force = 0 and Velocity of Centre of Mass = 0
Then centre of mass remains at rest. Individual components of a system may move and have non zero momentum due to mutual forces but the net momentum of the system remains zero.
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