In this question the box should be modelled as a particle.
A box of mass \(m\) kg is placed on a rough slope which makes an angle of \(\alpha\) with the horizontal.
- Show that the box is on the point of slipping if \(\mu = \tan \alpha\), where \(\mu\) is the coefficient of friction between the box and the slope. [2]
A box of mass 5 kg is pulled up a rough slope which makes an angle of 15° with the horizontal. The box is subject to a constant frictional force of magnitude 3 N. The speed of the box increases from 2 m s\(^{-1}\) at a point A on the slope to 5 m s\(^{-1}\) at a point B on the slope with B higher up the slope than A. The distance AB is 10 m.
\includegraphics{figure_6}
The pulling force has constant magnitude \(P\) N and acts at a constant angle of 25° above the slope, as shown in the diagram.
- Use the work–energy principle to determine the value of \(P\). [5]