
\[ T = S_1 \] \[ x_1 + y_1 y_1 = x_1^2 + y_1^2 \] It passes through \( (\alpha, 0) \), \[ \therefore \alpha x_1 = x_1^2 + y_1^2 \] \[ \alpha (2t^2) = 4t^4 + 16t^2 \quad \left( x_1 = 2t^2, y_1 = 4t \right) \] \[ \alpha = 2t^2 + 8 \] \[ t^2 = \frac{\alpha - 8}{2} \] \[ \Rightarrow \alpha > 8 \] Also, \[ 4t^2 + 16t^2 - 4 < 0 \quad \text{(point lies inside the circle)} \] \[ t^2 = -2 + \sqrt{5} \] \[ \alpha = 4 + 2\sqrt{5} \] \[ \therefore \alpha \in (8, 4 + 2\sqrt{5}) \] \[ \therefore (2q - p)^2 = 80 \]

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:\[ (2q - p)^2 = 80 \]

Two circular discs of radius \(10\) cm each are joined at their centres by a rod, as shown in the figure. The length of the rod is \(30\) cm and its mass is \(600\) g. The mass of each disc is also \(600\) g. If the applied torque between the two discs is \(43\times10^{-7}\) dyne·cm, then the angular acceleration of the system about the given axis \(AB\) is ________ rad s\(^{-2}\).
