Concept: This problem is based on the Principle of Conservation of Angular Momentum.
• Conservation of Angular Momentum: If no external torque acts on a system, the total angular momentum remains constant ($L_i = L_f$).
• Angular Momentum ($L$): Defined as $L = I\omega$, where $I$ is the moment of inertia and $\omega$ is the angular speed.
• Final System: When two discs are joined, they rotate together with a common angular speed $\omega_f$, and the total moment of inertia is the sum of their individual moments ($I_1 + I_2$).
Step 1: Set up the conservation equation.
Initial total angular momentum ($L_i$) is the sum of the individual momenta:
\[ L_i = I_1\omega_1 + I_2\omega_2 \]
Final total angular momentum ($L_f$) after they are brought together:
\[ L_f = (I_1 + I_2)\omega_f \]
According to the principle:
\[ I_1\omega_1 + I_2\omega_2 = (I_1 + I_2)\omega_f \]
Step 2: Substitute values and solve for $I_1$.
Given: $\omega_1 = 2 \text{ rads}^{-1}$, $\omega_2 = 5 \text{ rads}^{-1}$, $\omega_f = 4 \text{ rads}^{-1}$, and $I_2 = 1 \times 10^{-3} \text{ kg m}^2$.
\[ I_1(2) + (1 \times 10^{-3})(5) = (I_1 + 1 \times 10^{-3})(4) \]
\[ 2I_1 + 5 \times 10^{-3} = 4I_1 + 4 \times 10^{-3} \]
Rearranging terms:
\[ 5 \times 10^{-3} - 4 \times 10^{-3} = 4I_1 - 2I_1 \]
\[ 1 \times 10^{-3} = 2I_1 \]
\[ I_1 = \frac{1}{2} \times 10^{-3} = 0.5 \times 10^{-3} \text{ kg m}^2 \]