A particle of mass $m$, initially at rest, is acted on by a force $F = F_0 \left\{ {1 - {{\left( {\frac{{2t - T}}{T}} \right)}^2}} \right\}$ during the interval $0 \leq 0 \leq t \leq T$. The velocity of the particle at the end of the interval is :
A particle of mass $m$, initially at rest, is acted on by a force $F = F_0 \left\{ {1 - {{\left( {\frac{{2t - T}}{T}} \right)}^2}} \right\}$ during the interval $0 \leq 0 \leq t \leq T$. The velocity of the particle at the end of the interval is :
- A
$\frac{{5{F_0}T}}{{6m}}$
- B
$\frac{{4{F_0}T}}{{3m}}$
- C
$\frac{{2{F_0}T}}{{3m}}$
- D
$\frac{{3{F_0}T}}{{2m}}$
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