Write the expression of centre of mass of a system of $'n'$ particles and derive the formula of force acting on its centre of mass.
The centre of mass of a system of ' $n$ ' particle
$\vec{v}_{\mathrm{cm}} \text { or } \overrightarrow{\mathrm{V}}=\frac{m_{1} \overrightarrow{v_{1}}+m_{2} \overrightarrow{v_{2}}+\ldots m_{n} \overrightarrow{v_{n}}}{m_{1}+m_{2}+\ldots m_{n}}$
$\therefore \quad \mathrm{MV}=m_{1} \overrightarrow{v_{1}}+m_{2} \overrightarrow{v_{2}}+\ldots m_{n} \overrightarrow{v_{n}} \quad \ldots$
Where $\mathrm{M}=m_{1}+m_{2}+\ldots, m_{n}$ total mass of a system.
Assume that the value of masses does not change with time, then differentiate equation $(1)$ w.r.t. time,
$\mathrm{M} \frac{d \overrightarrow{\mathrm{V}}}{d t}=m_{1} \frac{d \overrightarrow{v_{1}}}{d t}+m_{2} \frac{d \overrightarrow{v_{2}}}{d t}+\ldots m_{n} \frac{d \overrightarrow{v_{n}}}{d t}$
but $\frac{d \overrightarrow{\mathrm{V}}}{d t}=\overrightarrow{\mathrm{A}}$ acceleration of centre of mass
$\frac{d \overrightarrow{v_{1}}}{d t}=\overrightarrow{a_{1}}$ acceleration of first particle
$\frac{d \overrightarrow{v_{2}}}{d t}=\overrightarrow{a_{2}}$ acceleration of second particle and
$\frac{d \overrightarrow{v_{n}}}{d t}=\overrightarrow{a_{n}}$ acceleration of ' $n$ ' particle
$\therefore \quad \mathrm{MA}=m_{1} \vec{a}_{1}+m_{2} \overrightarrow{a_{2}}+\ldots m_{n} \overrightarrow{a_{n}} \ldots$
OR
$\vec{a}_{\mathrm{cm}} \text { or } \overrightarrow{\mathrm{A}}=\frac{m_{1} \overrightarrow{a_{1}}+m_{2} \overrightarrow{a_{2}}+\ldots m_{n} \overrightarrow{a_{n}}}{m_{1}+m_{2}+\ldots m_{n}}$
is a formula for acceleration of centre of mass.
From Newton's second law, $\overrightarrow{\mathrm{F}}_{i}=m_{i} \vec{a}_{i}$ but $\mathrm{MA}=\overrightarrow{\mathrm{F}}_{1}+\overrightarrow{\mathrm{F}}_{2}+\ldots \overrightarrow{\mathrm{F}}_{n}$
Hence, the vector sum of all the forces acting on the all particles of a system is equal to the product of total mass of system and the acceleration of its centre of mass.
A uniform disc of radius $R$ is put over another uniform disc of radius $2R$ made of same material having same thickness.The peripheries of the two discs touches each other.Locate the centre of mass of the system taking center center of large disc at origin
In the figure shown a hole of radius $2\, cm$ is made in a semicircular disc of radius $6\pi$ at a distance $8 \,cm$ from the centre $C$ of the disc. The distance of the centre of mass of this system from point $C$ is ......... $cm$.
The centre of mass of a solid hemisphere of radius $8\, cm$ is $X \,cm$ from the centre of the flat surface. Then value of $x$ is$......$
From a uniform square plate, one-fourth part is removed as shown. The centre of mass of remaining part will lie on
As shown in figure, when a spherical cavity (centred at $\mathrm{O})$ of radius $1$ is cut out of a uniform sphere of radius $\mathrm{R} \text { (centred at } \mathrm{C}),$ the centre of mass of remaining (shaded) part of sphere is at $G$, i.e, on the surface of the cavity. $\mathrm{R}$ can be detemined by the equation