Step 1: Analyze energy conservation. At projection: \[ KE_i = \frac{1}{2}mv^2 \] At the highest point: \[ PE_f = mgh \quad {and} \quad KE_f = \frac{1}{2}mv_x^2 \] Where \( v_x = v \cos(30^\circ) \).
Step 2: Calculate the ratio. \[ v_x = v \cos(30^\circ) = v \cdot \frac{\sqrt{3}}{2} \] \[ KE_f = \frac{1}{2}m(v \cdot \frac{\sqrt{3}}{2})^2 = \frac{3}{8}mv^2 \] \[ {Ratio} = \frac{KE_i}{PE_f} = \frac{\frac{1}{2}mv^2}{mgh} \] Assuming \( h = \frac{v_y^2}{2g} \) and \( v_y = v \sin(30^\circ) = \frac{v}{2} \): \[ h = \frac{(\frac{v}{2})^2}{2g} = \frac{v^2}{8g} \] \[ PE_f = m \cdot \frac{v^2}{8g} \cdot g = \frac{mv^2}{8} \] \[ {Ratio} = \frac{\frac{1}{2}mv^2}{\frac{mv^2}{8}} = 4 \]
Find the least horizontal force \( P \) to start motion of any part of the system of three blocks resting upon one another as shown in the figure. The weights of blocks are \( A = 300 \, {N}, B = 100 \, {N}, C = 200 \, {N} \). The coefficient of friction between \( A \) and \( C \) is 0.3, between \( B \) and \( C \) is 0.2 and between \( C \) and the ground is 0.1.

If the roots of $\sqrt{\frac{1 - y}{y}} + \sqrt{\frac{y}{1 - y}} = \frac{5}{2}$ are $\alpha$ and $\beta$ ($\beta > \alpha$) and the equation $(\alpha + \beta)x^4 - 25\alpha \beta x^2 + (\gamma + \beta - \alpha) = 0$ has real roots, then a possible value of $y$ is: