Solution: For a circular orbit:
\[ \pi r^2 \propto \frac{L}{m}. \]
For planet A:
\[ \pi r_1^2 \cdot T_A \propto \frac{L}{2m_1}. \]
For planet B:
\[ \pi r_2^2 \cdot T_B \propto \frac{3L}{2m_2}. \]
Taking the ratio of time periods:
\[ \frac{T_A}{T_B} = \frac{m_2}{m_1} \cdot \left(\frac{r_1}{r_2}\right)^2. \]
Squaring both sides:
\[ \left(\frac{T_A}{T_B}\right)^2 = \frac{m_2^2}{m_1^2} \cdot \left(\frac{r_1}{r_2}\right)^4. \]
Taking the cube root:
\[ \frac{T_A}{T_B} = \frac{1}{27} \cdot \left(\frac{m_2}{m_1}\right)^3. \]
Final Answer: \(\frac{1}{27} \cdot \left(\frac{m_2}{m_1}\right)^3\).
A small point of mass \(m\) is placed at a distance \(2R\) from the center \(O\) of a big uniform solid sphere of mass \(M\) and radius \(R\). The gravitational force on \(m\) due to \(M\) is \(F_1\). A spherical part of radius \(R/3\) is removed from the big sphere as shown in the figure, and the gravitational force on \(m\) due to the remaining part of \(M\) is found to be \(F_2\). The value of the ratio \( F_1 : F_2 \) is:
Let the function, \(f(x)\) = \(\begin{cases} -3ax^2 - 2, & x < 1 \\a^2 + bx, & x \geq 1 \end{cases}\) Be differentiable for all \( x \in \mathbb{R} \), where \( a > 1 \), \( b \in \mathbb{R} \). If the area of the region enclosed by \( y = f(x) \) and the line \( y = -20 \) is \( \alpha + \beta\sqrt{3} \), where \( \alpha, \beta \in \mathbb{Z} \), then the value of \( \alpha + \beta \) is: