Varignon's theorem (mechanics) explained

Varignon's theorem is a theorem of French mathematician Pierre Varignon (1654–1722), published in 1687 in his book Projet d'une nouvelle mécanique. The theorem states that the torque of a resultant of two concurrent forces about any point is equal to the algebraic sum of the torques of its components about the same point. In other words, "If many concurrent forces are acting on a body, then the algebraic sum of torques of all the forces about a point in the plane of the forces is equal to the torque of their resultant about the same point."[1]

Proof

Consider a set of

N

force vectors

f1,f2,...,fN

that concur at a point

O

in space. Their resultant is:
N
F=\sum
i=1

fi

.

The torque of each vector with respect to some other point

O1

is
fi
\Tau
O1

=(O-O1) x fi

.

Adding up the torques and pulling out the common factor

(O-O1)
, one sees that the result may be expressed solely in terms of

F

, and is in fact the torque of

F

with respect to the point

O1

:
N
\sum
i=1
fi
\Tau
O1

=(O-O1) x \left(

N
\sum
i=1

fi\right) =(O-O1) x F =

F
\Tau
O1

.

Proving the theorem, i.e. that the sum of torques about

O1

is the same as the torque of the sum of the forces about the same point.

External links

Notes and References

  1. Book: Engineering Mechanics: Statics . I. C. Jong, B. G. Rogers . 1991. 9780030263095 .