Step 1. The equation of the circle is given as \( T = S_1 \), where:
\[ xx_1 + yy_1 = x_1^2 + y_1^2 \]
Step 2. Using the symmetry condition of the parabola and circle intersection:
\[ \alpha x_1 = x_1^2 + y_1^2 \]
Step 3. Substituting and simplifying:
\[ \alpha(2t^2) = 4t^4 + 16t^2 \]
Step 4. Rearranging:
\[ \alpha = 2t^2 + 8 \]
Step 5. Further refinement leads to:
\[ \frac{\alpha - 8}{2} = t^2 \]
Step 6. To ensure three distinct solutions, the discriminant condition for the quadratic is:
\[ 4t^4 + 16t^2 - 4 < 0 \]
Solving this gives:
\[ t^2 = -2 \pm \sqrt{5} \]
Step 7. Substituting back, \(\alpha\) lies in the interval:
\[ \alpha \in (8, 4 + 2\sqrt{5}) \]
Step 8. Hence, the values of \(p\) and \(q\) are:
\[ p = 8, \quad q = 4 + 2\sqrt{5} \]
Step 9. Finally, the value of \((2q - p)^2\) is:\[ (2q - p)^2 = 80 \]
As shown below, bob A of a pendulum having a massless string of length \( R \) is released from 60° to the vertical. It hits another bob B of half the mass that is at rest on a frictionless table in the center. Assuming elastic collision, the magnitude of the velocity of bob A after the collision will be (take \( g \) as acceleration due to gravity):