- A$754$
- B$654$
- ✓$294$
- D$354$
$ \left|\mathrm{f}_{\mathrm{c}}-\mathrm{f}_0\right|=7 $
$ \frac{\mathrm{v}}{4 \times 150}-\frac{\mathrm{v}}{2 \times 350}=7 $
$ \frac{\mathrm{v}}{600 \mathrm{~cm}}-\frac{\mathrm{v}}{700 \mathrm{~cm}}=7 $
$ \frac{\mathrm{v}}{6 \mathrm{~m}}-\frac{\mathrm{v}}{7 \mathrm{~m}}=7 $
$ \mathrm{v}\left(\frac{1}{42}\right)=7 $
$ \mathrm{v}=42 \times 7 $
$ =294 \mathrm{~m} / \mathrm{s}$
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$\rho=\left\{\begin{array}{l}\rho_0 \text { for } r \leq R \\ 0 \text { for } r>R\end{array}\right.$
where $\rho_0$ is a constant. A test mass can undergo circular motion under the influence of the gravitational field of particles. Its speed $V$ as a function of distance $\mathrm{r}(0<\mathrm{r}<\infty)$ from the centre of the system is represented by