MCQ
A particle of mass $M$ originally at rest is subjected to a force whose direction is constant but magnitude varies with time according to the relation
$F=F_{0}\left(1-\left(\frac{t-T}{T}\right)^{2}\right)$
Where $F_{0}$ and $T$ are constants. The force acts only for the time internal $2 T$. The velocity $v$ of the particle after time $2 {T}$ is -
- A$\frac{{F}_{0} {T}}{3 {M}}$
- B$\frac{{F}_{0} {T}}{2 {M}}$
- C$\frac{2{F}_{0} {T}}{{M}}$
- ✓$\frac{4 {F}_{0} {T}}{3 {M}}$
