Civil Engineering Reference
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which simplifies to
d 2
4
y 2
6 S y
bd 3
τ
=−
(10.7)
The distribution of vertical shear stress is therefore parabolic as shown in Fig. 10.5(b)
and varies from τ
=
0at y
d / 2to τ
=
τ max =
3 S y / 2 bd at the neutral axis ( y
=
0) of
the beam section. Note that τ max =
1 . 5 τ av , where τ av , the average vertical shear stress
over the section, is given by τ av =
S y / bd .
E XAMPLE 10.2 Determine the distribution of vertical shear stress in the I-section
beam of Fig. 10.6(a) produced by a vertical shear load, S y .
It is clear fromFig. 10.6(a) that the geometry of each of the areas A f and A w formed by
taking a slice of the beam in the flange (at y
y w ), respectively,
are different and will therefore lead to different distributions of shear stress. First we
shall consider the flange. The area A f is rectangular so that the distribution of vertical
shear stress, τ f , in the flange is, by direct comparison with Ex. 10.1
=
y f ) and in the web (at y
=
D
2
y f D
y f
S y
BI z
B
2
τ f =−
2 +
or
D 2
4
S y
2 I z
y f
τ f =−
(10.8)
where I z is the second moment of area of the complete section about the centroidal
axis G z and is obtained by the methods of Section 9.6.
A ' f
y
τ f at base
of flange
y f
A ' w
y w
z
d
D
τ max
G
t w
b
a
F IGURE 10.6 Shear
stress distribution in
an I-section beam
B
t f
(a)
(b)
 
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