Civil Engineering Reference
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S y
δ x
y
y 2
δ y
y
b 0
A
G
y 1
z
F IGURE 13.20 Determination of form
factor β
in which S is the applied shear force, A is the cross-sectional area of the beam section
and β is a constant which depends upon the distribution of shear stress through the
beam section; β is known as the form factor .
To determine β we consider an element b 0 δ
x of a beam
subjected to a vertical shear load S y (Fig. 13.20); we shall suppose that the beam
section has a vertical axis of symmetry. The shear stress τ is constant across the width,
b 0 , of the element (see Section 10.2). The strain energy,
y in an elemental length
δ
δ
U , of the element b 0 δ
y
δ
x ,
from Eq. (10.20) is
τ 2
2 G ×
δ
U
=
b 0 δ
y d x
(13.17)
Therefore the total strain energy U in the elemental length of beam is given by
y 2
x
2 G
δ
τ 2 b 0 d y
U
=
(13.18)
y 1
Alternatively U for the elemental length of beam is obtained using Eq. (13.16); thus
S y
A
2
β
2 G ×
U
=
×
A
δ
x
(13.19)
Equating Eqs (13.19) and (13.18) we have
S y
A
2
y 2
β
2 G ×
x
2 G
δ
τ 2 b 0 d y
×
A
δ
x
=
y 1
whence
y 2
A
S y
τ 2 b 0 d y
β
=
(13.20)
y 1
The shear stress distribution in a beam having a singly or doubly symmetrical cross
section and subjected to a vertical shear force, S y , is given by Eq. (10.4), i.e.
S y A ¯
y
=−
τ
b 0 I z
 
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