State and explain the law of conservation of momentum of the system of particle.
Newton's second law for the system of particle,
$\frac{d \vec{p}}{d t}=\overrightarrow{\mathrm{F}}_{\mathrm{ext}}$
If the sum of external forces acting on the system of particles is zero then
$\frac{d \vec{p}}{d t}=0$
$\therefore d \vec{p}=0, \therefore \overrightarrow{p_{1}}=\overrightarrow{p_{2}}$
Means the linear momentum remains constant.
$(\vec{p}=\text { constant })$
Equation $\vec{p}=$ constant, it is equivalent to three scalar equation as following :
$p_{x}=\mathrm{C}_{1}, p_{y}=\mathrm{C}_{2}, p_{3}=\mathrm{C}_{3}$
where $p_{x^{\prime}} p_{y}$ and $p_{z}$ are the components of linear momentum $\vec{p}$ for respective axis $\mathrm{X}, \mathrm{Y}$ and $\mathrm{Z}$ axis and $\mathrm{C}_{1}, \mathrm{C}_{2}$ and $\mathrm{C}_{3}$ are constant.
"When external total force acting on a system of particles is zero, then its total linear momentum remains constant." This is known as conservation of linear momentum.
From $\mathrm{MA}=\overrightarrow{\mathrm{F}}$, here $\overrightarrow{\mathrm{F}}$ is total external force.
If $\overrightarrow{\mathrm{F}}=0$ then $\overrightarrow{\mathrm{MA}}=0$
$\therefore \overrightarrow{\mathrm{A}}=0$
Means, "when total external force on system is zero, the velocity of centre of mass remains constant."
More over $\overrightarrow{\mathrm{A}}=\frac{d \vec{v}}{d t}$ then
If $\overrightarrow{\mathrm{A}}=0$ then $\frac{d \vec{v}}{d t}=0$
$\therefore \vec{v}$ is constant.
Means, total external force on the system is zero, the velocity of centre of mass remains constant.
Characteristic of rotational motion.
A sphere is rotating about a diameter
A solid sphere rotates about a vertical axis on frictionless bearing. A massless cord passes around the equator of sphere, then passes through over a solid cylinder and then is connected to block of mass $M$ as shown in figure. If the system is released from rest then the speed acquired by block after it has fallen through distance $h$ is
Why does the internal forces acting on the centre of mass of the system be neglected ?
A uniform solid cylinder of mass $M$ and radius $R$ rotates about a frictionless horizontal axle. Two similar masses suspended with the help two ropes wrapped around the cylinder. If the system is released from rest then the acceleration of each mass will be