Step 1. Calculate Initial Moment of Inertia and Kinetic Energy:
For the first disc:
\( I_1 = \frac{1}{2}MR^2 = \frac{1}{2} \times 5 \times (2)^2 = 10 \, \text{kg} \cdot \text{m}^2 \)
Initial angular velocity \( \omega = 10 \, \text{rad/s} \). Initial kinetic energy:
\( E_i = \frac{1}{2}I_1 \omega^2 = \frac{1}{2} \times 10 \times (10)^2 = 500 \, \text{J} \)
Step 2. Final Moment of Inertia and Angular Velocity:
When the second disc is placed on top, the combined moment of inertia becomes:
\( I_f = I_1 + I_2 = 10 + 10 = 20 \, \text{kg} \cdot \text{m}^2 \)
Using conservation of angular momentum:
\( I_1 \omega = I_f \omega_f \Rightarrow 10 \times 10 = 20 \times \omega_f \)
\( \omega_f = 5 \, \text{rad/s} \)
Step 3. Calculate Final Kinetic Energy:
\( E_f = \frac{1}{2} I_f \omega_f^2 = \frac{1}{2} \times 20 \times (5)^2 = 250 \, \text{J} \)
Step 4. Energy Dissipated:
Energy dissipated \( \Delta E = E_i - E_f \):
\( \Delta E = 500 - 250 = 250 \, \text{J} \)
A uniform circular disc of radius \( R \) and mass \( M \) is rotating about an axis perpendicular to its plane and passing through its center. A small circular part of radius \( R/2 \) is removed from the original disc as shown in the figure. Find the moment of inertia of the remaining part of the original disc about the axis as given above.
Let \( S = \left\{ m \in \mathbb{Z} : A^m + A^m = 3I - A^{-6} \right\} \), where
\[ A = \begin{bmatrix} 2 & -1 \\ 1 & 0 \end{bmatrix} \]Then \( n(S) \) is equal to ______.
The number of 6-letter words, with or without meaning, that can be formed using the letters of the word MATHS such that any letter that appears in the word must appear at least twice, is $ 4 \_\_\_\_\_$.
Let \( f : (0, \infty) \to \mathbb{R} \) be a twice differentiable function. If for some \( a \neq 0 \), } \[ \int_0^a f(x) \, dx = f(a), \quad f(1) = 1, \quad f(16) = \frac{1}{8}, \quad \text{then } 16 - f^{-1}\left( \frac{1}{16} \right) \text{ is equal to:}\]