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τ
A
B
τ
s AC τ
τ
s BD τ
D
C
τ
F IGURE 7.12 Stresses on diagonal planes in element
A
A
B
B
45 ° approx
F
f
f
F IGURE 7.13 Distortion due to shear in
element
D
C
Hence we see that on planes parallel to the diagonals of the element there are direct
stresses σ BD (tensile) and σ AC (compressive) both numerically equal to τ as shown
in Fig. 7.12. It follows from Section 7.8 that the direct strain in the direction BD is
given by
σ BD
E
νσ AC
E
τ
E (1
ε BD =
+
=
+
ν )
(7.18)
Note that the compressive stress σ AC makes a positive contribution to the strain ε BD .
In Section 7.5 we defined shear strain and saw that under pure shear, only a change
of shape is involved. Thus the element ABCD of Fig. 7.11(a) distorts into the shape
A B CD shown in Fig. 7.13. The shear strain γ produced by the shear stress τ is then
given by
B B
BC
γ
=
φ radians
=
(7.19)
since φ is a small angle. The increase in length of the diagonal DB to DB
is
approximately equal to FB where BF is perpendicular to DB . Thus
DB
FB
DB
DB
ε DB =
=
DB
Again, since φ is a small angle, B B F
45 so that
FB =
BB cos 45
 
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