To solve the problem, we need to determine the ratio of the total flying times \( T_1 \) and \( T_2 \) of two balls projected at different angles but with the same initial velocity, given that the maximum height of the first ball is 8 times that of the second ball.
\(H = \frac{v_i^2 \sin^2 \theta}{2g}\)
\(T = \frac{2v_i \sin \theta}{g}\)
\(\frac{H_1}{H_2} = 8\)
\(\frac{\frac{v_i^2 \sin^2 \theta_1}{2g}}{\frac{v_i^2 \sin^2 \theta_2}{2g}} = 8\)
\(\frac{\sin^2 \theta_1}{\sin^2 \theta_2} = 8\)
\(\frac{T_1}{T_2} = \frac{\frac{2v_i \sin \theta_1}{g}}{\frac{2v_i \sin \theta_2}{g}} = \frac{\sin \theta_1}{\sin \theta_2}\)
\(\frac{\sin^2 \theta_1}{\sin^2 \theta_2} = 8\)
\(\frac{\sin \theta_1}{\sin \theta_2} = \sqrt{8} = 2\sqrt{2}\)
Therefore, the ratio of the total flying times \( T_1 \) and \( T_2 \) is \( 2\sqrt{2} : 1 \).
Two light beams fall on a transparent material block at point 1 and 2 with angle \( \theta_1 \) and \( \theta_2 \), respectively, as shown in the figure. After refraction, the beams intersect at point 3 which is exactly on the interface at the other end of the block. Given: the distance between 1 and 2, \( d = 4/3 \) cm and \( \theta_1 = \theta_2 = \cos^{-1} \frac{n_2}{2n_1} \), where \( n_2 \) is the refractive index of the block and \( n_1 \) is the refractive index of the outside medium, then the thickness of the block is cm. 
A bob of mass \(m\) is suspended at a point \(O\) by a light string of length \(l\) and left to perform vertical motion (circular) as shown in the figure. Initially, by applying horizontal velocity \(v_0\) at the point ‘A’, the string becomes slack when the bob reaches at the point ‘D’. The ratio of the kinetic energy of the bob at the points B and C is: 
Two light beams fall on a transparent material block at point 1 and 2 with angle \( \theta_1 \) and \( \theta_2 \), respectively, as shown in the figure. After refraction, the beams intersect at point 3 which is exactly on the interface at the other end of the block. Given: the distance between 1 and 2, \( d = \frac{4}{3} \) cm and \( \theta_1 = \theta_2 = \cos^{-1} \left( \frac{n_2}{2n_1} \right) \), where \( n_2 \) is the refractive index of the block and \( n_1 \) is the refractive index of the outside medium, then the thickness of the block is …….. cm.

Let \( y^2 = 12x \) be the parabola and \( S \) its focus. Let \( PQ \) be a focal chord of the parabola such that \( (SP)(SQ) = \frac{147}{4} \). Let \( C \) be the circle described by taking \( PQ \) as a diameter. If the equation of the circle \( C \) is: \[ 64x^2 + 64y^2 - \alpha x - 64\sqrt{3}y = \beta, \] then \( \beta - \alpha \) is equal to: