Step 1: State Kepler's Third Law of planetary motion. For objects orbiting the same central body, the square of the orbital period (\(T\)) is directly proportional to the cube of the semi-major axis of its orbit. For a circular orbit, this is the radius (\(r\)). \[ \frac{T^2}{r^3} = \text{constant} \]
Step 2: Set up a ratio for the two satellites. Let \(T_1, r_1\) be the period and radius for the first satellite, and \(T_2, r_2\) for the second. \[ \frac{T_1^2}{r_1^3} = \frac{T_2^2}{r_2^3} \]
Step 3: Rearrange the formula to solve for the unknown period, \(T_2\). \[ T_2^2 = T_1^2 \left( \frac{r_2}{r_1} \right)^3 \] \[ T_2 = T_1 \left( \frac{r_2}{r_1} \right)^{3/2} \]
Step 4: Substitute the given values and calculate \(T_2\). - \( T_1 = 3 \) hours - \( r_1 = 12000 \) km - \( r_2 = 48000 \) km The ratio of the radii is \( \frac{r_2}{r_1} = \frac{48000}{12000} = 4 \). \[ T_2 = 3 \times (4)^{3/2} = 3 \times (\sqrt{4})^3 = 3 \times (2)^3 = 3 \times 8 = 24 \text{ hours} \]
If \(f(t)\) is the inverse Laplace transform of \( F(s) = \frac{s+1+s^{-2}}{s^2-1} \), then \(f(t)\) is
Match LIST-I with LIST-II
LIST-I (Differential Equation)
(A) \(\frac{dy}{dx} = 2x(y-x^2+1)\)
(B) \(x\frac{dy}{dx} + 2(x^2+1)y=6\)
(C) \((x^2+1)\frac{dy}{dx} + 2xy = x \sin x\)
(D) \(x^3\frac{dy}{dx} + 2xy = 2x^2e^{x^2}\)
LIST-II (Integrating Factor)
(I) \(x^2\)
(II) \(e^{-x^2}\)
(III) \(x^2e^x\)
(IV) \(1+x^2\)
Choose the correct answer from the options given below: