The speed \(v\) of a satellite in a circular orbit is given by the formula: \[ v = \sqrt{\frac{GM}{r}} \] Where: - \(G\) is the gravitational constant, - \(M\) is the mass of the planet, - \(r\) is the radius of the orbit. Let the speed of satellite A be \(v_A\) and the speed of satellite B be \(v_B\). For satellite A, the radius of orbit is \(2R\), and for satellite B, the radius is \(R\). From the formula, we know that the speed of satellite A is: \[ v_A = \sqrt{\frac{GM}{2R}} = 2v \] Now, using the same formula for satellite B: \[ v_B = \sqrt{\frac{GM}{R}} \] Using the ratio of the speeds: \[ \frac{v_B}{v_A} = \frac{\sqrt{\frac{GM}{R}}}{\sqrt{\frac{GM}{2R}}} = \sqrt{2} \] Therefore: \[ v_B = v_A \cdot \sqrt{2} = 2v \cdot \sqrt{2} = 2\sqrt{2}v \]
Thus, the speed of satellite B is \( 2\sqrt{2}v \).
The correct option is (B) : \(2\sqrt2v\)
Let the gravitational force provide the necessary centripetal force for a satellite in circular orbit.
For a satellite of mass m orbiting at radius r around a planet of mass M, the balance of forces gives:
$$ \frac{G M m}{r^2} = \frac{m v^2}{r} $$
Canceling m and simplifying:
$$ \frac{G M}{r} = v^2 $$
So, $$ v = \sqrt{\frac{G M}{r}} $$
Speed is inversely proportional to the square root of the radius: $$ v \propto \frac{1}{\sqrt{r}} $$
Let the radius of satellite A be \( r_A = 2R \) and speed be \( v_A = 2v \). Let the radius of satellite B be \( r_B = R \) and speed be \( v_B \).
Using the proportionality: $$ \frac{v_B}{v_A} = \sqrt{\frac{r_A}{r_B}} = \sqrt{\frac{2R}{R}} = \sqrt{2} $$
So, $$ v_B = v_A \cdot \sqrt{2} = 2v \cdot \sqrt{2} = 2\sqrt{2}v $$
Correct answer: 2√2v
Net gravitational force at the center of a square is found to be \( F_1 \) when four particles having masses \( M, 2M, 3M \) and \( 4M \) are placed at the four corners of the square as shown in figure, and it is \( F_2 \) when the positions of \( 3M \) and \( 4M \) are interchanged. The ratio \( \dfrac{F_1}{F_2} = \dfrac{\alpha}{\sqrt{5}} \). The value of \( \alpha \) is 
