Civil Engineering Reference
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the point. Thus, in Fig. 2.12, the moment, M ,of F about O is given by
M
=
Fa
(2.5)
where ' a ' is known as the lever arm or moment arm of F about O; note that the units
of a moment are the units of force
×
distance.
It can be seen from the above that a moment possesses both magnitude and a rota-
tional sense. For example, in Fig. 2.12, F exerts a clockwise moment about O. A
moment is therefore a vector (an alternative argument is that the product of a vec-
tor, F , and a scalar, a , is a vector). It is conventional to represent a moment vector
graphically by a double-headed arrow, where the direction of the arrow designates a
clockwise moment when looking in the direction of the arrow. Therefore, in Fig. 2.12,
the moment M (
Fa ) would be represented by a double-headed arrow through Owith
its direction into the plane of the paper.
=
Moments, being vectors, may be resolved into components in the same way as forces.
Consider the moment, M (Fig. 2.13(a)), in a plane inclined at an angle θ to the xz
plane. The component of M in the xz plane, M xz , may be imagined to be produced
by rotating the plane containing M through the angle θ into the xz plane. Similarly,
the component of M in the yz plane, M yz , is obtained by rotating the plane containing
M through the angle 90
θ . Vectorially, the situation is that shown in Fig. 2.13(b),
where the directions of the arrows represent clockwise moments when viewed in the
directions of the arrows. Then
M xz =
M cos θ M yz =
M sin θ
The action of a moment on a structural member depends upon the plane in which it
acts. For example, in Fig. 2.14(a), the moment, M , which is applied in the longitu-
dinal vertical plane of symmetry, will cause the beam to bend in a vertical plane. In
Fig. 2.14(b) the moment, M , is applied in the plane of the cross section of the beam
and will therefore produce twisting; in this case M is called a torque .
y
M yz
M xz M cos u
M
M
M xz
x
u
u
F IGURE 2.13
Resolution of a
moment
z
M yz M sin u
(a)
(b)
 
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