To determine what is conserved when a child sits on a rotating disc, we must consider the physical principles involved. The scenario involves rotational motion, so the concept of angular momentum is key.
Angular momentum is defined as the product of the moment of inertia and angular velocity. The formula for angular momentum \(L\) for a rotating object is:
\(L = I \cdot \omega\)
where:
In the absence of external torques, angular momentum is conserved according to the law of conservation of angular momentum. This means that the total angular momentum of a system remains constant if no external forces are acting on it.
When the child sits on the rotating disc, the system's moment of inertia changes due to the added mass of the child. As a result, the angular speed \(\omega\) will adjust to keep the angular momentum \(L\) constant, provided no external torque is acting on the system.
Now, let’s evaluate the options:
The correct answer is that angular momentum is conserved when a child sits on the rotating disc, given no external torques act on the system.
The center of mass of a thin rectangular plate (fig - x) with sides of length \( a \) and \( b \), whose mass per unit area (\( \sigma \)) varies as \( \sigma = \sigma_0 \frac{x}{ab} \) (where \( \sigma_0 \) is a constant), would be 