To determine at which time the torque on a rotating wheel becomes zero, we start with the given function for the angular position of a point on the wheel:
The angular position $\theta(t) = 2t^3 - 6t^2$.
The angular velocity $\omega(t)$ is the first derivative of angular position with respect to time:
$\omega(t) = \frac{d\theta}{dt} = \frac{d}{dt}(2t^3 - 6t^2)$
Calculating the derivative:
$\omega(t) = 6t^2 - 12t$
The angular acceleration $\alpha(t)$ is the derivative of angular velocity:
$\alpha(t) = \frac{d\omega}{dt} = \frac{d}{dt}(6t^2 - 12t)$
Calculating the derivative:
$\alpha(t) = 12t - 12$
The torque $\tau$ is related to the angular acceleration by the equation:
$\tau = I \alpha$, where $I$ is the moment of inertia.
Since we are looking for when the torque is zero, we need:
$0 = I(12t - 12)$
For the torque to be zero, the angular acceleration must be zero:
$12t - 12 = 0$
Solve for $t$:
$12t = 12$
$t = 1$ second.
Hence, the torque on the wheel becomes zero at t = 1 s.