To solve this problem, we need to calculate the escape velocity from planet \(B\) given the information about its density and radius relative to planet \(A\).
Step 1: Understand the Escape Velocity Formula
The formula for escape velocity \(v_e\) from a planet is given by:
\(v_e = \sqrt{\frac{2GM}{R}}\)
Where:
We also know that mass \(M\) is related to density \(\rho\) and volume \(V\) (which is a function of radius \(R\)) as follows:
\(M = \rho \cdot V = \rho \cdot \frac{4}{3} \pi R^3\)
Substituting this into the escape velocity formula, we get:
\(v_e = \sqrt{\frac{2G \rho \cdot \frac{4}{3} \pi R^3}{R}} = \sqrt{\frac{8}{3} \pi G \rho R^2}\)
Step 2: Calculate the Escape Velocity for Planet \(B\)
From the problem, the density and radius of planet \(B\) are \(10\%\) of those of planet \(A\), therefore:
The escape velocity for planet \(B\) becomes:
\(v_{eB} = \sqrt{\frac{8}{3} \pi G \cdot (0.1 \rho_A) \cdot (0.1 R_A)^2}\)
\(v_{eB} = \sqrt{0.1^3 \cdot \frac{8}{3} \pi G \rho_A R_A^2}\)
Therefore, we have:
\(v_{eB} = 0.1^{3/2} \cdot v_{eA}\)
Step 3: Substitute the Given Values
Given that the escape velocity from planet \(A\), \(v_{eA} = 10 \ \text{km/s} = 10000\ \text{m/s}\), we substitute:
\(v_{eB} = 0.1^{3/2} \cdot 10000\)
\(v_{eB} = 0.1^{3/2} \cdot 10000 = 0.1^{1.5} \cdot 10000\)
\(v_{eB} = 0.0316227766 \cdot 10000 = 316.227766\ \text{m/s} \cdot \sqrt{10}\)
Simplifying, we get:
\(v_{eB} = 1000\sqrt{2}\ \text{m/s}\)
Conclusion
The escape velocity from planet \(B\) is \(1000\sqrt{2}\ \text{m/s}\).
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 
