- A$\frac{1}{2}\,m{\omega ^2}x$
- B$\frac{1}{2}\,m{\omega ^2}\frac{{{x^2}}}{l}$
- C$\frac{1}{2}\,m{\omega ^2}l\,\left( {1 - \frac{x}{l}} \right)$
- ✓$\frac{1}{2}\,\frac{{m{\omega ^2}}}{l}\,\left( {{l^2} - {x^2}} \right)$
The force on the element towards the axis $=T-(T+d T)=-d T$
$\therefore-d T=(d m) \omega^{2} x=\left(\frac{m}{l} d x\right) \omega^{2} x$
$T=-\frac{m \omega^{2}}{l} \cdot \frac{x^{2}}{2}+$ constant
For $x=1, T=0 . \quad \therefore$ the constant $=\frac{1}{2} \cdot \frac{m \omega^{2} l^{2}}{l}$
$\therefore T=\frac{1}{2} \cdot \frac{m \omega^{2}}{l}\left(l^{2}-x^{2}\right)$
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