
To solve this problem, we need to understand the motion of the particle P as it revolves around the center O in a circular path with radius r and angular velocity \omega. We are focusing on the projection of the line OP on the x-axis at a given time t.
The general formula for the projection of a revolving vector on an axis is based on the angle it makes with the reference axis. Here, the angle is given by the angular displacement \theta = \omega t.
From the diagram provided, the particle P starts its motion at an initial angle of \frac{\pi}{6} (30 degrees), going counterclockwise.
The x-coordinate of the particle can therefore be determined by considering both the angular velocity and the initial phase:
Hence, the correct expression for the projection of OP on the x-axis at time t is:
Thus, the correct option is:
This solution accounts for the initial phase angle introduced in the problem, providing a precise mathematical representation of the motion.
A body of mass 1000 kg is moving horizontally with a velocity of 6 m/s. If 200 kg extra mass is added, the final velocity (in m/s) is: