The cylinder is acted upon by the force of gravity m1g, the normal reaction N1 of the left

inclined plane, and the normal reaction N3 of the wedge (force N3 has the horizontal direction). We shall write the equation of motion of the cylinder in terms of projections on the x1-axis directed along the left inclined plane (Fig. 153):

where a1 is the projection of the acceleration of the cylinder on the x1 - axis.
The wedge is acted upon by the force of gravity m2g, the normal reaction N2 of the right inclined plane, and the normal reaction of the cylinder, which, according to Newton's third law, is equal to - N3. We shall write the equation of motion of the wedge in terms of projections on the x1-axis directed along the right inclined plane:

During its motion, the wedge is in contact with the cylinder. Therefore, if the displacement of the wedge along the x1-axis is Δx, the centre of the cylinder (together with the vertical face of the wedge) will be displaced along the horizontal by Δx cos a. The centre of the cylinder will be thereby displaced along the left inclined plane (x1-axis) by Δx. This means that in the process of motion of the wedge and the cylinder, the relation

is satisfied.
Solving Eqs. (1) - (3) simultaneously, we determine the force of normal pressure N = N3 exerted by the wedge on the cylinder:
