Obtain Newton's second law for system of particle and write it. 

Vedclass pdf generator app on play store
Vedclass iOS app on app store

Linear momentum of system of particle

$\vec{p}=m \vec{v}$

Taking differention on both side with time

$\frac{d \vec{p}}{d t}=\mathrm{M} \frac{d \vec{v}}{d t}$ (where $\mathrm{M}=$ constant $)$

$\therefore \frac{d \vec{p}}{d t}=\mathrm{MA}$

$\ldots$ (2)

but $\overrightarrow{\mathrm{MA}}=\overrightarrow{\mathrm{F}}_{\mathrm{ext}}$

From equation (2) and (3),

$\frac{d \vec{p}}{d t}=\overrightarrow{\mathrm{F}}_{\mathrm{ext}}$

is a Newton's second law for the system of particles.

"The external force acting on a system is equal to rate of change of total linear momentum of the system." This is Newton's second law for a system.

Similar Questions

There is a rod of lenght $l$, mass $m$ lying on a fixed horizontal smooth table. A cord is led through a pulley, and its horizontal part is attached to one end of the rod, while its vertical part is attached to a block of mass $m_1$.  Assume pulley and the cord is ideal. The maximum possible acceleration of the rod's centre of mass $C$ (for all possible values of masses $m$ and $m_1$) at the moment of releasing the block $m_1$ is $\frac{g}{n}$.  Find the value of $n$

 

What is rigid body?

Explain with illustration the pure translation and combination of translation and rotation motion of rigid body.

In the given figure linear acceleration of solid cylinder of mass $m_2$ is $a_2$. Then angular acceleration $\alpha_2$ is (given that there is no slipping).

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