Overconstrained mechanism

An overconstrained mechanism is a linkage that has more degrees of freedom than is predicted by the mobility formula. The mobility formula evaluates the degree of freedom of a system of rigid bodies that results when constraints are imposed in the form of joints between the links.

The crank-driven elliptic trammel is an overconstrained mechanism.

If the links of the system move in three-dimensional space, then the mobility formula is

${\displaystyle M=6(N-1-j)+\sum _{i=1}^{j}f_{i},}$

where N is the number of links in the system, j is the number of joints, and fi is the degree of freedom of the ith joint.

If the links in the system move planes parallel to a fixed plane, or in concentric spheres about a fixed point, then the mobility formula is

${\displaystyle M=3(N-1-j)+\sum _{i=1}^{j}f_{i}.}$

If a system of links and joints has mobility ${\displaystyle M=0}$ or less, yet still moves, then it is called an overconstrained mechanism.

Reason of over-constraint

A hinged door is one of the simplest over-constrained mechanism.

The reason of over-constraint is the unique geometry of linkages in these mechanisms, which the mobility formula does not take into account. This unique geometry gives rise to "redundant constraints", i.e. when multiple joints are constraining the same degrees of freedom. These redundant constraints are the reason of the over-constraint.

For example, as shown in the figure to the right, consider a hinged door with 3 hinges. The mobility criterion for this door gives the mobility to be zero. Yet, the door moves and has a degree of freedom 1, as all its hinges are constraining the same degrees of freedom.

Examples of over-constrained mechanisms

A well-known example of an overconstrained mechanism is the parallel linkage with multiple cranks, as seen in the running gear of steam locomotives.

Sarrus mechanism consists of six bars connected by six hinged joints.

A general spatial linkage formed from six links and six hinged joints has mobility

${\displaystyle M=6(N-1-j)+\sum _{i=1}^{j}f_{i}=6(6-1-6)+6=0,}$

and is therefore a structure.

The Sarrus mechanism has one degree of freedom whereas the mobility formula yields M = 0, which means it has a particular set of dimensions that allow movement.[1]

Another example of an overconstrained mechanism is Bennett's linkage, which consists of four links connected by four revolute joints.[2]

A general spatial linkage formed from four links and four hinged joints has mobility

${\displaystyle M=6(N-1-j)+\sum _{i=1}^{j}f_{i}=6(4-1-4)+4=-2,}$

which is a highly constrained system.

As in the case of the Sarrus linkage, it is a particular set of dimensions that makes the Bennett linkage movable.[3][4]

The dimensional constraints that makes Bennett's linkage movable are the following. Let us number the links in order that links with consecutive index are joined (first and fourth links are also joined). For the i-th link, let us denote by di and ai respectively the distance and the oriented angle of the axes of the revolute joints of the link. Bennett's linkage must satisfies the following constraints:

{\displaystyle {\begin{aligned}&d_{1}=d_{3},\quad a_{1}=a_{3}\\&d_{2}=d_{4},\quad a_{2}=a_{4}\\&{\frac {d_{1}^{2}}{sin^{2}a_{1}}}={\frac {d_{2}^{2}}{sin^{2}a_{2}}}.\end{aligned}}}

Moreover, the links are assembled in such a way that, for two links that are joined together, the common perpendicular to the joint axes of the first link intersects the common perpendicular of the joint axes of the second link.

Below is an external link to an animation of a Bennett's linkage.

Hoberman mechanism

Same as the crank-driven elliptic trammel, Hoberman mechanisms move because of their particular geometric configurations.