The energy consumed by the motor is the change in rotational kinetic energy. The rotational kinetic energy is given by:
\[
E = \frac{1}{2} I \omega^2
\]
where \( I \) is the moment of inertia and \( \omega \) is the angular velocity.
The angular velocity \( \omega \) is related to the speed \( N \) in RPM by:
\[
\omega = \frac{2\pi N}{60}
\]
Given:
- Inertia \( I = 0.1 \, \text{kg-m}^2 \),
- Initial speed \( N_1 = 1000 \, \text{RPM} \),
- Final speed \( N_2 = 1500 \, \text{RPM} \).
The initial and final angular velocities are:
\[
\omega_1 = \frac{2\pi \times 1000}{60} = \frac{1000\pi}{30} = 104.72 \, \text{rad/s}
\]
\[
\omega_2 = \frac{2\pi \times 1500}{60} = \frac{1500\pi}{30} = 157.08 \, \text{rad/s}
\]
Now, calculate the initial and final kinetic energies:
\[
E_1 = \frac{1}{2} \times 0.1 \times (104.72)^2 = 548.35 \, \text{J}
\]
\[
E_2 = \frac{1}{2} \times 0.1 \times (157.08)^2 = 1231.65 \, \text{J}
\]
The energy consumed by the motor is the difference:
\[
\Delta E = E_2 - E_1 = 1231.65 - 548.35 = 683.3 \, \text{J}
\]
Thus, the energy consumed by the motor is approximately \( 675 \, \text{J} \) (rounded to nearest integer).