The torque or moment of a force
about a point is the cross product of the vector
from the point in question to point of application of the force with the force, that is![]()
For example, the moment of
acting at
about the point
is


Properties:
The moment is at right angles to both
and
This is a consequence of the cross product. In the above diagram the moment is directed out of the paper, since the cross product defines a right handed coordinate system.
If a force acts at a point, the moment of the force about that point is zero.
The total moment of a system of forces is equal to the sum of the moments:![]()
The Total Moment is a vector, with magnitude given by
where
is the acute angle between
and![]()