
The diagram shows a mechanism for converting rotational motion into linear motion. The point \(P\) is on the circumference of a disc of fixed radius r which can rotate about a fixed point \(O\). The point \(Q\) can only move on the line \(OX\), and \(P\) and \(Q\) are connected by a rod of length \(2r\). As the disc rotates, the point \(Q\) is made to slide along \(OX\). At time t, angle \(POQ\) is \(\theta\) and the distance \(OQ\) is \(x\).
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