To solve this problem, we need to consider the conservation of angular momentum. Since the platform is mounted on a frictionless vertical axle, the total angular momentum of the man-platform system remains constant. Let us break down the problem step-by-step:
The initial angular momentum of the system is zero because both the man and platform are initially at rest.
When the man starts walking on the platform, he will have an angular momentum about the axis of rotation given by:
Due to conservation of angular momentum, the platform will rotate in the opposite direction to maintain zero net angular momentum.
Let the angular velocity of the platform be \omega. The angular momentum of the platform is then:
Using the principle of conservation of angular momentum, where the initial angular momentum is equal to the final angular momentum, we have:
The man will walk one complete revolution in time T using the formula:
However, note that due to the effect of the platform's rotation, taking rid of the simplifying condition:
The correct answer is 2 \pi \, s.
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 