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BULETINUL INSTITUTULUI POLITEHNIC DIN IAŞI

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36 Radu Ibănescu and Cătălin Ungureanu<br />

Φ<br />

d<br />

F<br />

B<br />

h<br />

C<br />

A<br />

l<br />

R<br />

M m<br />

e<br />

O<br />

ϕ (t)<br />

G<br />

a<br />

Fig. 1 – Eccentric cam.<br />

h i<br />

diagram is obtained showing the dependence of the cam follower length with<br />

respect to the moment acting on the cam, so that the cam follower does not<br />

stick. The required length of the cam follower guide can be chosen from this<br />

diagram.<br />

2. The Eccentric Cam Mechanism<br />

The eccentric cam mechanism consists of a disk of radius R actuated by a<br />

couple M m (Fig. 1). The disk can rotate about the fix point O located at the<br />

distance e from the centre of the circle. The cam follower is vertical and it has a<br />

horizontal bar at each of its ends. The bar at the bottom end lies on the cam. The<br />

bar at the top end is actuated by a spring having the spring stiffness k e and by a<br />

constant force F collinear to the spring. The disk weight is G and the weight of<br />

the cam follower is assumed to be very small and hence negligible.<br />

The friction coefficient between the cam follower and the disk and the<br />

cam follower and its guide is μ. The friction coefficient in the joint at O is μ 1 .<br />

All the dimensions are known and can be seen in Fig. 1. The problem is to<br />

determine the minimum value of the driving couple M m to maintain the<br />

mechanism in equilibrium at limit state. The disk and the cam follower are

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