- A$\frac{3}{5}\,Mv_0R$
- B$\frac{4}{5}\,Mv_0R$
- ✓$\frac{7}{5}\,Mv_0R$
- D$\frac{7}{2}\,Mv_0R$
here $v_{\mathrm{cm}}=v_0$
since sphere is in pure rolling motion hence $\omega=\mathrm{v}_{0} / \mathrm{R}$
$\Rightarrow \vec{\mathrm{L}}_{\mathrm{p}}=\left(\frac{2}{5} \mathrm{MR}^{2} \frac{\mathrm{v}_{0}}{\mathrm{R}}\right)(-\hat{\mathrm{k}})+\mathrm{M} \mathrm{v}_{\mathrm{o}} \mathrm{R}(-\hat{\mathrm{k}})$
$=\frac{7}{5} \mathrm{Mv}_{0} \mathrm{R}(-\hat{\mathrm{k}})$
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$\mathrm{MSR}=8.45 \mathrm{~cm}, \mathrm{VC}=26$
For mark on paper seen through slab
$\mathrm{MSR}=7.12 \mathrm{~cm}, \mathrm{VC}=41$
For powder particle on the top surface of the glass slab
$\mathrm{MSR}=4.05 \mathrm{~cm}, \mathrm{VC}=1$
$(\mathrm{MSR}=$ Main Scale Reading, $\mathrm{VC}=$ Vernier Coincidence)
Refractive index of the glass slab is:
